[go: up one dir, main page]

TW202240006A - Conformal and smooth titanium nitride layers and methods of forming the same - Google Patents

Conformal and smooth titanium nitride layers and methods of forming the same Download PDF

Info

Publication number
TW202240006A
TW202240006A TW110146342A TW110146342A TW202240006A TW 202240006 A TW202240006 A TW 202240006A TW 110146342 A TW110146342 A TW 110146342A TW 110146342 A TW110146342 A TW 110146342A TW 202240006 A TW202240006 A TW 202240006A
Authority
TW
Taiwan
Prior art keywords
tin
precursor
thin film
flow rate
ratio
Prior art date
Application number
TW110146342A
Other languages
Chinese (zh)
Inventor
趙賢哲
金海英
阿傑特 丹希爾
佈生 B 聶
鄭昇勳
Original Assignee
美商尤金納斯股份有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 美商尤金納斯股份有限公司 filed Critical 美商尤金納斯股份有限公司
Publication of TW202240006A publication Critical patent/TW202240006A/en

Links

Images

Classifications

    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/22Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the deposition of inorganic material, other than metallic material
    • C23C16/30Deposition of compounds, mixtures or solid solutions, e.g. borides, carbides, nitrides
    • C23C16/34Nitrides
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/04Coating on selected surface areas, e.g. using masks
    • C23C16/045Coating cavities or hollow spaces, e.g. interior of tubes; Infiltration of porous substrates
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/455Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • C23C16/45523Pulsed gas flow or change of composition over time
    • C23C16/45525Atomic layer deposition [ALD]
    • C23C16/45527Atomic layer deposition [ALD] characterized by the ALD cycle, e.g. different flows or temperatures during half-reactions, unusual pulsing sequence, use of precursor mixtures or auxiliary reactants or activations
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/455Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • C23C16/45523Pulsed gas flow or change of composition over time
    • C23C16/45525Atomic layer deposition [ALD]
    • C23C16/45553Atomic layer deposition [ALD] characterized by the use of precursors specially adapted for ALD
    • CCHEMISTRY; METALLURGY
    • C23COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23CCOATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C16/00Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
    • C23C16/44Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating
    • C23C16/455Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the method of coating characterised by the method used for introducing gases into reaction chamber or for modifying gas flows in reaction chamber
    • C23C16/45557Pulsed pressure or control pressure
    • H10D64/01318
    • H10P14/432
    • H10W20/033

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • General Chemical & Material Sciences (AREA)
  • Chemical Kinetics & Catalysis (AREA)
  • Materials Engineering (AREA)
  • Mechanical Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Chemical Vapour Deposition (AREA)
  • Electrodes Of Semiconductors (AREA)
  • Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)
  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Manufacturing & Machinery (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Composite Materials (AREA)

Abstract

The disclosed technology generally relates to forming a thin film comprising titanium nitride (TiN), and more particularly to forming by a cyclical vapor deposition process the thin film comprising (TiN). In one aspect, a method a method of forming a thin film comprising titanium nitride (TiN) by a cyclical vapor deposition process comprises forming on a semiconductor substrate a TiN thin film by exposing the semiconductor substrate to one or more cyclical vapor deposition cycles each comprising an exposure to a Ti precursor at a Ti precursor flow rate and an exposure to a N precursor at a N precursor flow rate, wherein a ratio of the N precursor flow rate to the Ti precursor flow rate exceeds 3. The method is such that the TiN thin film has a preferential (111) crystalline texture such that an X-ray spectrum of the TiN thin film has a ratio of a peak height or an intensity of an X-ray diffraction peak corresponding to a (111) crystal orientation of TiN to a peak height or an intensity of an X-ray diffraction peak corresponding to a (200) crystal orientation of TiN that exceeds 0.4. Aspects are also directed to semiconductor structures incorporating the thin film and method of forming the same.

Description

保形且平滑之氮化鈦層及其形成方法Conformal and smooth titanium nitride layer and method of forming same

本發明大體上係關於形成氮化鈦層,且更特定言之係關於保形且平滑之氮化鈦層。The present invention relates generally to forming titanium nitride layers, and more particularly to conformal and smooth titanium nitride layers.

氮化鈦(TiN)已被廣泛用於積體電路(IC)中之各種結構之製造。例如,TiN已用於擴散阻障、各種電極及金屬化結構。TiN在IC製造中之此廣泛使用可歸因於其結構、熱及電性質。隨著各種IC結構之尺寸縮小,TiN經形成於具有愈來愈小之尺寸及複雜拓撲之特徵上。例如,隨著技術節點按比例調整至10 nm節點且甚至更小,需要可保形地加襯裡於具有小至幾奈米之尺寸之高縱橫比溝渠及通孔之TiN層(例如,作為擴散阻障)。儘管數十年來在IC產業中已使用諸如物理氣相沈積(PVD)及化學氣相沈積(CVD)之技術來形成TiN,但對將沈積於較小溝渠或通孔中之TiN膜之保形性之經增加需求可最終限制其等之使用。另一方面,雖然已證實原子層沈積(ALD)用於TiN膜之保形沈積,但該膜之一些電性質(例如,導電率)及實體性質(例如,表面粗糙度)相較於使用諸如物理氣相沈積(PVD)之其他方法形成之TiN膜可能較差。因此,需要用於形成用於IC製造中之相對於藉由PVD及CVD形成之TiN膜具有優越表面平滑度及階梯覆蓋率同時亦具有匹配或優越電及實體性質之以TiN為主之膜之原子層沈積方法。Titanium nitride (TiN) has been widely used in the fabrication of various structures in integrated circuits (ICs). For example, TiN has been used in diffusion barriers, various electrodes and metallization structures. This widespread use of TiN in IC fabrication can be attributed to its structural, thermal and electrical properties. As the dimensions of various IC structures shrink, TiN is formed on features with increasingly smaller dimensions and complex topologies. For example, as technology nodes scale to the 10 nm node and beyond, there is a need for TiN layers that can conformally line high aspect ratio trenches and vias with dimensions as small as a few nanometers (e.g., as diffusion barrier). Although techniques such as physical vapor deposition (PVD) and chemical vapor deposition (CVD) have been used in the IC industry for decades to form TiN, the conformal The increased demand for sex can ultimately limit their use. On the other hand, while atomic layer deposition (ALD) has been demonstrated for conformal deposition of TiN films, some electrical properties (e.g., conductivity) and physical properties (e.g., surface roughness) of the films are comparable to those obtained using methods such as TiN films formed by other methods of physical vapor deposition (PVD) may be inferior. Accordingly, there is a need for methods for forming TiN-based films for use in IC fabrication that have superior surface smoothness and step coverage relative to TiN films formed by PVD and CVD, while also having matching or superior electrical and physical properties. Atomic layer deposition method.

在一項態樣中,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括至第一Ti前驅體之暴露及至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環而在該半導體基板上形成該薄膜之第一部分。此外,該方法包括藉由使該半導體基板暴露至各包括至第二Ti前驅體之暴露及至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在該薄膜之該第一部分上形成該薄膜之第二部分。相對於在該一或多個第一ALD循環期間至Ti前驅體及N前驅體之一或兩者之對應暴露,在該一或多個第二ALD循環期間至該Ti前驅體及該N前驅體之一或兩者之暴露係在較高壓力下。In one aspect, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes exposing a semiconductor substrate to respective exposures to a first Ti precursor and to a first N The exposure of the precursor to one or more first periodic vapor deposition cycles forms a first portion of the thin film on the semiconductor substrate. Additionally, the method includes exposing the semiconductor substrate to one or more second periodic vapor deposition cycles each comprising exposure to a second Ti precursor and exposure to a second N precursor to the A second portion of the film is formed on the first portion. The exposure to the Ti precursor and the N precursor during the one or more second ALD cycles relative to the corresponding exposure to one or both of the Ti precursor and the N precursor during the one or more first ALD cycles The exposure of one or both bodies is under higher pressure.

在另一態樣中,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括提供包括具有超過1之縱橫比之溝渠或通孔之半導體基板。此外,該方法包括藉由使該半導體基板暴露至各包括至第一Ti前驅體之暴露及至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環以在該溝渠或該通孔中形成該薄膜之第一部分而在該溝渠或該通孔中形成該薄膜。此外,該方法包括使該半導體基板暴露至各包括至第二Ti前驅體之暴露及至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環以在該薄膜之該第一部分上形成該薄膜之第二部分。相對於在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之對應暴露,在該一或多個第一週期性氣相沈積循環期間至該第一Ti前驅體及該第一N前驅體之一或兩者之暴露係在不同壓力下。In another aspect, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes providing a semiconductor substrate comprising trenches or vias having an aspect ratio greater than one. Additionally, the method includes exposing the semiconductor substrate to one or more first periodic vapor deposition cycles each including exposure to a first Ti precursor and exposure to a first N precursor A first portion of the film is formed in the via and the film is formed in the trench or the via. In addition, the method includes exposing the semiconductor substrate to one or more second periodic vapor deposition cycles each comprising exposure to a second Ti precursor and exposure to a second N precursor to deposit the first portion of the thin film A second portion of the film is formed thereon. Relative to the corresponding exposure to one or both of the second Ti precursor and the second N precursor during the one or more second periodic vapor deposition cycles, during the one or more first periodic Exposure to one or both of the first Ti precursor and the first N precursor during a vapor deposition cycle is at different pressures.

在另一態樣中,一種半導體結構包括半導體基板,該半導體基板包括在具有超過5之縱橫比之溝渠或通孔中之非金屬側壁表面。此外,該半導體結構包括保形地塗佈該非金屬側壁表面之包括TiN之薄膜,其中形成於該溝渠或該通孔之高度之下25%及該溝渠或該通孔之該高度之上25%上之該薄膜之厚度之比率超過0.9。In another aspect, a semiconductor structure includes a semiconductor substrate including non-metallic sidewall surfaces in trenches or vias having an aspect ratio exceeding 5. In addition, the semiconductor structure includes a thin film comprising TiN conformally coating the non-metallic sidewall surface, wherein formed below 25% of the height of the trench or the via and above 25% of the height of the trench or the via The ratio of the thickness of the film above exceeds 0.9.

在另一態樣中,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜,其中該N前驅體流動速率與該Ti前驅體流動速率之比率超過3。該方法使得該TiN薄膜具有優先(111)結晶紋理,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。In another aspect, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes exposing a semiconductor substrate to a Ti precursor at a Ti precursor flow rate and forming a TiN thin film on the semiconductor substrate at one or more periodic vapor deposition cycles of N precursor flow rate to N precursor exposure, wherein the ratio of the N precursor flow rate to the Ti precursor flow rate More than 3. The method makes the TiN thin film have a preferential (111) crystal texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) corresponding to TiN. The ratio of the peak height or intensity of the X-ray diffraction peaks of the crystal orientation to more than 0.4.

在另一態樣中,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜,其中該N前驅體流動速率超過500 sccm。該方法使得該TiN薄膜具有優先(111)結晶紋理,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。In another aspect, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes exposing a semiconductor substrate to a Ti precursor at a Ti precursor flow rate and one or more periodic vapor deposition cycles of exposure to N precursor at a N precursor flow rate to form a TiN film on the semiconductor substrate, wherein the N precursor flow rate exceeds 500 sccm. The method makes the TiN thin film have a preferential (111) crystal texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) corresponding to TiN. The ratio of the peak height or intensity of the X-ray diffraction peaks of the crystal orientation to more than 0.4.

在另一態樣中,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜。此外,該方法包括藉由使該半導體基板暴露至各包括以第二Ti前驅體流動速率至第二Ti前驅體之暴露及以第二N前驅體流動速率至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在該TiN薄膜上形成第二TiN薄膜。該方法使得該TiN薄膜及該第二TiN薄膜之一或兩者具有優先(111)結晶紋理,使得該TiN薄膜及該第二TiN薄膜之一或兩者之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。In another aspect, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes exposing a semiconductor substrate to a Ti precursor at a Ti precursor flow rate and one or more periodic vapor deposition cycles of exposure to the N precursor at the N precursor flow rate to form a TiN thin film on the semiconductor substrate. Additionally, the method includes exposing the semiconductor substrate to one of exposure to a second Ti precursor at a second Ti precursor flow rate and exposure to a second N precursor at a second N precursor flow rate by exposing the semiconductor substrate to or a plurality of second periodic vapor deposition cycles to form a second TiN thin film on the TiN thin film. The method makes one or both of the TiN thin film and the second TiN thin film have a preferential (111) crystal texture, so that the X-ray spectrum of one or both of the TiN thin film and the second TiN thin film has a corresponding TiN ( 111) The ratio of the peak height or intensity of the X-ray diffraction peak of the crystal orientation to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN exceeds 0.4.

在另一態樣中,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括以第一Ti前驅體流動速率至第一Ti前驅體之暴露及以第一N前驅體流動速率至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環而在第一壓力下在該半導體基板上形成第一TiN薄膜。該第一TiN薄膜具有結晶紋理,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。此外,該方法包括藉由使該半導體基板暴露至各包括以第二Ti前驅體流動速率至第二Ti前驅體之暴露及以第二N前驅體流動速率至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在高於該第一壓力之第二壓力下在該第一TiN薄膜上形成第二TiN薄膜。In another aspect, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes exposing a semiconductor substrate to a temperature each comprising a first Ti precursor flow rate to a first TiN Precursor exposure and one or more first periodic vapor deposition cycles of exposure to the first N precursor at a first N precursor flow rate to form a first TiN thin film on the semiconductor substrate at a first pressure . The first TiN thin film has a crystalline texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the X-ray corresponding to the (200) crystal orientation of TiN The ratio of the peak height or intensity of diffraction peaks exceeding 0.4. Additionally, the method includes exposing the semiconductor substrate to one of exposure to a second Ti precursor at a second Ti precursor flow rate and exposure to a second N precursor at a second N precursor flow rate by exposing the semiconductor substrate to or a plurality of second periodic vapor deposition cycles to form a second TiN film on the first TiN film at a second pressure higher than the first pressure.

在另一態樣中,一種半導體結構包括半導體基板,該半導體基板包括在具有超過5之縱橫比之溝渠或通孔中之非金屬側壁表面。此外,該半導體結構包括保形地塗佈該非金屬側壁表面之包括TiN之薄膜,其中該薄膜具有優先(111)結晶紋理,使得該薄膜之X射線繞射輪廓具有對應於(111)晶向之X射線繞射峰之峰值高度或強度與對應於(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。In another aspect, a semiconductor structure includes a semiconductor substrate including non-metallic sidewall surfaces in trenches or vias having an aspect ratio exceeding 5. Additionally, the semiconductor structure includes a thin film comprising TiN conformally coating the non-metallic sidewall surface, wherein the thin film has a preferential (111) crystallographic texture such that the X-ray diffraction profile of the thin film has an orientation corresponding to a (111) crystallographic orientation The ratio of the peak height or intensity of the X-ray diffraction peak to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation exceeds 0.4.

任何優先申請案之引用併入Incorporation by reference of any priority application

在如與本申請案一起申請之申請案資料表中識別其外籍或國內優先權主張之任何及所有申請案根據37 CFR 1.57規定以引用的方式併入本文。Any and all applications for which foreign or domestic priority claims are identified in the Application Data Sheet as filed with this application are hereby incorporated by reference pursuant to 37 CFR 1.57.

本申請案係於2019年10月8日申請之標題為「CONFORMAL AND SMOOTH TITANIUM NITRIDE LAYERS AND METHODS OF FORMING THE SAME」之美國申請案第16/595,945之部分接續申請案,該案根據35 U.S.C. § 119(e)規定主張2020年12月10日申請之標題為「CONFORMAL AND SMOOTH TITANIUM NITRIDE LAYERS AND METHODS OF FORMING THE SAME」之美國臨時專利申請案第63/123,733號之優先權利,各案之全部內容以引用的方式明確併入本文。This application is a continuation-in-part of U.S. Application Serial No. 16/595,945, filed October 8, 2019, entitled "CONFORMAL AND SMOOTH TITANIUM NITRIDE LAYERS AND METHODS OF FORMING THE SAME," pursuant to 35 U.S.C. § 119 (e) To claim priority to U.S. Provisional Patent Application No. 63/123,733, filed on December 10, 2020, entitled "CONFORMAL AND SMOOTH TITANIUM NITRIDE LAYERS AND METHODS OF FORMING THE SAME," the entire contents of which are The manner of reference is expressly incorporated herein.

如上文所描述,積體電路(IC)產業中需要具有優越電及實體性質之平滑且保形TiN膜,以及形成此等膜之方法。為解決此等及其他需求,本文中揭示包括TiN之平滑且保形薄膜,及形成該薄膜之週期性氣相沈積方法,此薄膜顯示藉由週期性氣相沈積程序沈積之膜之保形性特性,同時亦具有優於或匹配藉由現有物理氣相沈積(PVD)及化學氣相沈積(CVD)方法形成之TiN膜之電及實體性質之電及實體性質。特定言之,形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括至第一Ti前驅體之暴露及至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環而在該半導體基板上形成該薄膜之第一部分。此外,該方法包括藉由使半導體基板暴露至各包括至第二Ti前驅體之暴露及至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在該薄膜之該第一部分上形成該薄膜之第二部分。相較於在該一或多個第一週期性氣相沈積循環期間至該第一Ti前驅體及該第一N前驅體之一或兩者之對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之暴露係不同的。本文中所揭示之週期性氣相沈積程序有時被稱為原子層沈積(ALD)。然而,週期性氣相沈積程序並不限於原子層沈積程序。例如,在本文中所描述之各項實施例中,前驅體可使反應表面部分或實質上飽和。As described above, there is a need in the integrated circuit (IC) industry for smooth and conformal TiN films with superior electrical and physical properties, and methods of forming such films. To address these and other needs, disclosed herein are smooth and conformal thin films comprising TiN, and periodic vapor deposition methods for forming such films that exhibit conformality of films deposited by periodic vapor deposition procedures characteristics, while also having electrical and physical properties superior to or matching those of TiN films formed by existing physical vapor deposition (PVD) and chemical vapor deposition (CVD) methods. In particular, the method of forming a thin film comprising titanium nitride (TiN) includes exposing a semiconductor substrate to one or more first periods each comprising exposure to a first Ti precursor and exposure to a first N precursor A permanent vapor deposition cycle is used to form a first portion of the thin film on the semiconductor substrate. In addition, the method includes exposing the semiconductor substrate to one or more second periodic vapor deposition cycles each comprising exposure to a second Ti precursor and exposure to a second N precursor on the first A second portion of the film is formed on one portion. During the one or more second periodic cycles, compared to the corresponding exposure to one or both of the first Ti precursor and the first N precursor during the one or more first periodic vapor deposition cycles, during the one or more second periodic cycles Exposure to one or both of the second Ti precursor and the second N precursor is varied during the active vapor deposition cycle. The periodic vapor deposition process disclosed herein is sometimes referred to as atomic layer deposition (ALD). However, periodic vapor deposition procedures are not limited to atomic layer deposition procedures. For example, in various embodiments described herein, the precursor can partially or substantially saturate the reaction surface.

藉由在薄膜之第一部分之沈積期間在相對較低壓力(例如,小於3托)下使基板暴露至Ti及/或N前驅體,初始膜生長可實質上以逐層生長模式繼續進行,此有利地導致相對於藉由在較高壓力(例如,大於3托或5托)下使基板暴露至Ti及/或N前驅體而沈積之可比較TiN膜較低之平均晶粒大小及表面粗糙度。另一方面,藉由在薄膜之第二部分之沈積期間在相對較高壓力(例如,大於3托)下使基板暴露至Ti及/或N前驅體,膜生長之後一部分有利地導致相對於藉由在相對較低壓力(例如,小於3托或小於1托)下使基板暴露至Ti及/或N前驅體而沈積之可比較TiN膜較高之保形度或階梯覆蓋率。By exposing the substrate to Ti and/or N precursors at relatively low pressures (e.g., less than 3 Torr) during deposition of the first portion of the thin film, initial film growth can proceed substantially in a layer-by-layer growth mode, whereby Advantageously results in lower average grain size and surface roughness relative to comparable TiN films deposited by exposing the substrate to Ti and/or N precursors at higher pressures (e.g., greater than 3 Torr or 5 Torr) Spend. On the other hand, by exposing the substrate to Ti and/or N precursors at relatively high pressures (e.g., greater than 3 Torr) during deposition of the second portion of the thin film, a portion after film growth advantageously results in Comparable TiN films deposited from exposing substrates to Ti and/or N precursors at relatively low pressures (eg, less than 3 Torr or less than 1 Torr) have higher conformality or step coverage.

另外,相較於以在相對較高壓力下暴露至Ti及/或N前驅體開始而生長之可比較薄膜,由於TiN膜之第一部分以逐層模式生長,故薄膜之第二部分可使用第一部分作為模板以逐層模式生長。Additionally, since the first portion of the TiN film is grown in a layer-by-layer mode, the second portion of the film can be grown using the second A portion acts as a template to grow in a layer-by-layer pattern.

作為最終結果,當沈積於特定表面(例如,包括非金屬表面之表面)上時,包括藉由根據本文中所揭示之方法在用於Ti前驅體及N前驅體之一或兩者之兩個不同對應暴露壓力下沈積而沈積之第一及第二部分之薄膜有利地具有優於使用單一壓力形成於相同表面上之薄膜層之表面粗糙度及保形性之組合。替代性地或此外,部分歸因於改良之平滑度及保形性,薄膜具有相較於藉由一些現有方法形成之TiN層相對較低之電阻率。As a final result, when deposited on a specific surface (e.g., a surface including a non-metallic surface), including by using methods according to the methods disclosed herein for one or both of the Ti precursor and N precursor The thin films of the first and second portions deposited at different corresponding exposure pressures advantageously have a combination of surface roughness and conformality superior to thin film layers formed on the same surface using a single pressure. Alternatively or additionally, due in part to the improved smoothness and conformality, the thin films have relatively lower resistivity compared to TiN layers formed by some prior methods.

如本文中所描述,除非明確限制,否則由其構成元素所指之不具有其特定化學計量比之化合物應被理解為涵蓋各元素之所有可能非零濃度。例如,氮化鈦(TiN)應被理解為涵蓋可由通式Ti xN表達之氮化鈦之所有可能化學計量及非化學計量組合物,其中x>0,包含TiN、Ti 3N 4、Ti 4N 3、Ti 6N 5、Ti 2N及TiN 2以及Ti及N之其他非化學計量組合物。 As described herein, unless expressly limited, a compound referred to by its constituent elements not having their specific stoichiometric ratios should be understood to encompass all possible non-zero concentrations of the respective elements. For example, titanium nitride (TiN) should be understood to cover all possible stoichiometric and non-stoichiometric compositions of titanium nitride that can be expressed by the general formula Ti x N, where x > 0, including TiN, Ti 3 N 4 , Ti 4 N 3 , Ti 6 N 5 , Ti 2 N and TiN 2 and other non-stoichiometric compositions of Ti and N.

如上文所描述,氮化鈦(TiN)在積體電路(IC)製造中發揮重要作用。雖然在IC產業中已使用諸如物理氣相沈積(PVD)及化學氣相沈積(CVD)之技術來沈積TiN,但對用於形成具有高保形性而不會顯著損害電及實體性質之以TiN為主之膜之沈積方法之需求已日益增加。As described above, titanium nitride (TiN) plays an important role in integrated circuit (IC) fabrication. Although techniques such as Physical Vapor Deposition (PVD) and Chemical Vapor Deposition (CVD) have been used in the IC industry to deposit TiN, it is difficult to use TiN for forming TiN with high conformality without significant damage to electrical and physical properties. There has been an increasing demand for methods of deposition of films based on these materials.

另外,雖然諸如電漿增強型原子層沈積(PE-ALD)之電漿增強型程序可有效地在具有相對較低縱橫比之表面上形成保形膜,但此等程序可能無法有效地在具有相對較高縱橫比之通孔及腔內部沈積膜。在不受理論約束之情況下,針對此之一個可能原因在於,在一些境況下,電漿或其活性物種可能無法到達高縱橫比通孔之較深部分。在此等境況中,通孔之不同部分可暴露至不同量之電漿或其活性物種,從而導致非均勻沈積之非所要結構效應,諸如相較於較深部分(有時被稱為尖化或鍵孔形成),在通孔之開口附近沈積較厚膜。由於此等原因,熱ALD可更為有利,因為熱ALD不取決於電漿或其活性物種到達其所沈積之表面之部分之能力。Additionally, while plasma-enhanced processes such as plasma-enhanced atomic layer deposition (PE-ALD) are effective in forming conformal films on surfaces with relatively low aspect ratios, such processes may not be effective on surfaces with Relatively high aspect ratio vias and deposited films inside cavities. Without being bound by theory, one possible reason for this is that, under some circumstances, the plasma or its active species may not be able to reach the deeper portions of the high aspect ratio vias. In these circumstances, different parts of the via may be exposed to different amounts of plasma or its active species, leading to undesired structural effects of non-uniform deposition, such as sharpening compared to deeper parts (sometimes referred to as peaking). or keyhole formation), a thicker film is deposited near the opening of the via. For these reasons, thermal ALD can be more advantageous because thermal ALD does not depend on the ability of the plasma or its active species to reach the portion of the surface on which it is deposited.

然而,雖然熱ALD技術可適於在形貌(尤其具有相對較高縱橫比(例如,超過1:1)之形貌)上形成相對保形TiN膜,但本發明者已認識到,藉由熱ALD形成之TiN膜在某些方面(例如,膜粗糙度及電阻率)可不如藉由PVD或CVD形成之TiN膜。在此方面,本發明者已發現,ALD生長之以TiN為主之膜之一些電性質及/或實體性質可受生長模式影響。特定言之,本發明者已發現,雖然可期望在ALD中以二維逐層生長模式生長以TiN為主之膜,但在一些境況下可能不容易達成此逐層生長模式。本發明者已進一步發現,藉由ALD以逐層生長模式生長以TiN為主之膜在IC製造中提出特定挑戰,其中在非金屬表面(尤其絕緣表面(諸如氧化物及氮化物表面)或半導體表面(諸如經摻雜及無摻雜矽表面))上形成以TiN為主之膜。本發明者已認識到,可以逐層生長模式生長以TiN為主之膜之程度可繼而取決於初始生長模式,該初始生長模式取決於表面之類型,如本文中參考圖1A至圖1D所描述,而不欲受任何理論約束。However, while thermal ALD techniques may be suitable for forming relatively conformal TiN films on topography, especially topography with relatively high aspect ratios (e.g., exceeding 1:1), the inventors have realized that by TiN films formed by thermal ALD may be inferior to TiN films formed by PVD or CVD in certain aspects, such as film roughness and resistivity. In this regard, the inventors have discovered that some electrical and/or physical properties of ALD grown TiN-based films can be affected by the growth mode. In particular, the inventors have discovered that while it may be desirable to grow TiN-dominated films in ALD in a two-dimensional layer-by-layer growth mode, this layer-by-layer growth mode may not be readily achievable in some circumstances. The present inventors have further discovered that the growth of TiN-dominated films by ALD in layer-by-layer growth mode presents particular challenges in IC fabrication, where on non-metallic surfaces, especially insulating surfaces such as oxide and nitride surfaces, or semiconductor TiN-dominated films are formed on surfaces such as doped and undoped silicon surfaces. The inventors have realized that the extent to which TiN-dominated films can be grown in a layer-by-layer growth mode may in turn depend on the initial growth mode, which depends on the type of surface, as described herein with reference to FIGS. 1A-1D , without wishing to be bound by any theory.

圖1A示意性地繪示TiN層之成核且圖1B至圖1D繪示TiN層在不同表面上之不同生長模式。參考圖1A,一旦前驅體分子104到達基板100之表面,其等便實體地吸附於該表面上。一些經吸附分子104可沿著基板100之表面擴散直至其等到達待化學吸附之能量上有利位置。該表面擴散尤其係由基板溫度、基板材料及經吸附分子之動能來管理。當藉由經化學吸附分子形成之核之大小超過藉由體積自由能與表面能之間的權衡而判定之特定大小(有時被稱為「臨界大小」)時,核可變得能量上穩定,且開始在大小上生長。因此,穩定核之如此形成之層108藉由併入額外前驅體分子104而繼續生長。後續膜生長可根據在圖1B至圖1D中示意性地繪示之不同生長模式分類。Figure 1A schematically depicts the nucleation of a TiN layer and Figures 1B-1D depict different growth modes of the TiN layer on different surfaces. Referring to FIG. 1A, once the precursor molecules 104 reach the surface of the substrate 100, they are physically adsorbed on the surface. Some of the adsorbed molecules 104 may diffuse along the surface of the substrate 100 until they wait to reach energetically favorable sites to be chemisorbed. The surface diffusion is governed inter alia by the substrate temperature, the substrate material and the kinetic energy of the adsorbed molecules. When the size of the nucleus formed by chemisorbed molecules exceeds a certain size (sometimes referred to as the "critical size") determined by the trade-off between bulk free energy and surface energy, the nucleus can become energetically stable , and begin to grow in size. Thus, the thus formed layer 108 of stable nuclei continues to grow by incorporating additional precursor molecules 104 . Subsequent film growth can be classified according to different growth modes schematically depicted in Figures 1B-1D.

圖1B示意性地繪示導致三維島狀物之層112之形成之三維島狀生長模式(有時被稱為Volmer–Weber生長模式)。在不受任何理論約束之情況下,當與三維島狀物相關聯之淨表面自由能為正時,該島狀生長模式可佔主導地位,從而指示與結合至基板相比,經沈積原子更牢固地彼此結合。將瞭解,例如,當TiN金屬層沈積在一些半導體及/或絕緣材料表面上時,TiN層之ALD生長之能量學可有利於島狀生長模式。Figure IB schematically depicts the three-dimensional island growth pattern (sometimes referred to as the Volmer-Weber growth pattern) leading to the formation of a layer 112 of three-dimensional islands. Without being bound by any theory, when the net surface free energy associated with a three-dimensional island is positive, the island growth mode can dominate, indicating that deposited atoms are more deposited than bound to the substrate. firmly bonded to each other. It will be appreciated that the energetics of ALD growth of a TiN layer may favor an island growth mode, for example, when a TiN metal layer is deposited on some semiconductor and/or insulating material surfaces.

圖1C繪示導致相對平滑二維層116之形成之逐層生長模式(有時被稱為Frank-van der Merwe生長模式)。在不受任何理論約束之情況下,當與彼此結合相比,經沈積原子更牢固地結合至基板時,該逐層生長模式可佔主導地位,使得能量上有利於穩定二維層116。當層之間的結合能量自第一單層至TiN層之體晶值連續降低時,可維持逐層生長模式。FIG. 1C illustrates a layer-by-layer growth mode (sometimes referred to as the Frank-van der Merwe growth mode) that results in the formation of a relatively smooth two-dimensional layer 116 . Without being bound by any theory, this layer-by-layer growth mode may dominate when the deposited atoms are more strongly bound to the substrate than to each other, making it energetically favorable to stabilize the two-dimensional layer 116 . The layer-by-layer growth mode can be maintained when the bonding energy between layers decreases continuously from the first monolayer to the bulk crystal value of the TiN layer.

雖然圖1B及圖1C係薄膜之兩種不同可能生長模式,但將瞭解,在一些境況下,在逐層生長模式與三維生長模式中間之生長模式係可能的。圖1D繪示被稱為Stranski-Krastanov (SK)生長模式之中間生長模式之實例。在不受任何理論約束之情況下,SK生長可發生在以逐層模式開始之薄膜生長中。當逐層生長在形成一或多個單層之後變得不利時,島狀生長模式開始主導優勢高於逐層生長模式,從而導致其中在二維初始層上形成三維島狀物之薄膜結構120。SK生長模式可作為應變鬆弛機制(應變引發之粗糙化)發生。While FIGS. 1B and 1C are two different possible growth modes for thin films, it will be appreciated that in some circumstances growth modes intermediate between layer-by-layer and three-dimensional growth modes are possible. Figure ID shows an example of an intermediate growth pattern known as the Stranski-Krastanov (SK) growth pattern. Without being bound by any theory, SK growth can occur in thin film growth starting in layer-by-layer mode. When layer-by-layer growth becomes unfavorable after the formation of one or more monolayers, the island growth mode becomes dominant over the layer-by-layer growth mode, resulting in a thin-film structure in which three-dimensional islands are formed on a two-dimensional initial layer 120 . The SK growth mode can occur as a strain relaxation mechanism (strain-induced roughening).

除了沈積物與基板之間的相互作用之外,其他因素(諸如基板溫度、反應器壓力及沈積速率)可顯著影響成核及早期生長程序,此繼而影響所得薄膜之最終奈米結構或微結構。例如,增強表面擴散之沈積條件(例如,相對較高基板溫度、相對較低壓力及/或較低沈積速率)可促進以逐層模式生長。因此,如本文中所揭示,藉由(例如)憑藉降低壓力及生長速率來增強在TiN膜之初始部分之沈積期間之表面擴散,根據實施例之初始膜生長可實質上以逐層生長模式繼續進行。In addition to the interaction between the deposit and the substrate, other factors such as substrate temperature, reactor pressure, and deposition rate can significantly affect the nucleation and early growth process, which in turn affects the final nanostructure or microstructure of the resulting film . For example, deposition conditions that enhance surface diffusion (eg, relatively higher substrate temperatures, relatively lower pressures, and/or lower deposition rates) can promote growth in a layer-by-layer mode. Thus, as disclosed herein, initial film growth according to embodiments may continue substantially in a layer-by-layer growth mode by, for example, enhancing surface diffusion during deposition of the initial portion of the TiN film by reducing pressure and growth rate conduct.

據發現,當藉由ALD在IC製造中所關注之各種表面(諸如介電質及半導體表面)上生長TiN時,ALD生長以三維島狀生長模式或SK生長模式初始化。例如,在一些境況下,在包含經摻雜及無摻雜之Si、SiO 2、Si 3N 4及其他高K或低K材料之基板表面上之TiN之ALD生長可以島狀生長模式或SK生長模式繼續進行。本發明者已發現,部分歸因於島狀生長模式或SK生長模式之初始生長模式,藉由ALD之TiN之後續生長通常導致對於用於高縱橫比結構之超薄保形TiN之各種應用非所要之膜形態,如圖2中所繪示。 It was found that when TiN is grown by ALD on various surfaces of interest in IC fabrication, such as dielectric and semiconductor surfaces, ALD growth is initiated in a three-dimensional island growth mode or SK growth mode. For example, in some circumstances, ALD growth of TiN on the surface of a substrate comprising doped and undoped Si, SiO2 , Si3N4, and other high - K or low - K materials can be in island growth mode or SK Growth mode continues. The present inventors have found that, due in part to the initial growth mode of the island growth mode or the SK growth mode, subsequent growth of TiN by ALD generally results in ultrathin conformal TiN for various applications that are useful for high aspect ratio structures. The desired film morphology is as shown in FIG. 2 .

圖2係藉由熱ALD生長於用原生氧化物塗佈之Si基板上之TiN層之橫截面透射電子顯微照片。在以三維島狀或SK生長模式生長之初始膜之後,TiN之ALD生長通常藉由具有不同定向之相鄰晶體之競爭性生長特性化,在一些境況下,其導致接近於成核層之V形晶粒且最終以較高膜厚度形成柱狀形態。如圖2中所繪示,所得膜形態包含引起顯著表面粗糙度之琢面柱頂及相對於晶粒具有較低密度之柱邊界。將瞭解,該等柱邊界相對於晶粒本身可具有顯著更差之擴散阻障性質,且可用作用於將非所要污染物輸送通過TiN層之最小電阻之路徑。Figure 2 is a cross-sectional transmission electron micrograph of a TiN layer grown by thermal ALD on a Si substrate coated with native oxide. After an initial film grown in a three-dimensional island or SK growth mode, ALD growth of TiN is usually characterized by the competitive growth of adjacent crystals with different orientations, which in some cases results in a V close to that of the nucleation layer. shape grains and eventually form columnar morphology with higher film thickness. As depicted in Figure 2, the resulting film morphology includes faceted pillar tops causing significant surface roughness and pillar boundaries with a lower density relative to the grains. It will be appreciated that such pillar boundaries may have significantly poorer diffusion barrier properties relative to the grains themselves, and may serve as the path of least resistance for transporting unwanted contaminants through the TiN layer.

本發明者已發現,當藉由在相對較低壓力(例如,小於1托)下使基板暴露至Ti及/或N前驅體而在非金屬表面上形成TiN層之初始部分時,在TiN沈積之初始階段(例如,成核階段)中可抑制初始三維或SK生長模式且可促進逐層生長模式。除其他原因外,此可是因為,經吸附之Ti及N前驅體分子之局部擴散具有更多時間來局部擴散且以相對較低接觸角潤濕基板表面(尤其非金屬表面)。在相對較低暴露壓力下生長之TiN層導致均勻地覆蓋大面積之該非金屬表面而實質上未形成島狀物之層,使得初始生長階段更傾向於有利於在基板表面上之逐層生長模式,在基板表面上,ALD TiN通常將有利於如上所述之三維島狀或SK生長模式。因此,藉由憑藉在相對較低前驅體暴露壓力(例如,小於3托)下使基板暴露至Ti及/或N前驅體來起始TiN之ALD,所得初始層可以逐層模式生長(例如,在成核階段中)。可藉由在相對較高前驅體暴露壓力(例如,大於3托)下使基板暴露至Ti及/或N前驅體而繼續進行之後續塊體生長階段可繼續以逐層模式進行。藉由採用根據實施例之方法,可避免TiN之習知ALD之一些缺點,尤其在藉由ALD在一些半導體及/或絕緣材料(尤其包括Si、SiO 2及/或Si 3N 4之無機層)上直接形成TiN層時,此通常可與藉由如上所述之島狀或SK生長模式接著進行柱狀生長特性化之初始生長相關聯。 The present inventors have discovered that when an initial portion of a TiN layer is formed on a non-metallic surface by exposing the substrate to Ti and/or N precursors at relatively low pressures (e.g., less than 1 Torr), The initial three-dimensional or SK growth mode can be suppressed and the layer-by-layer growth mode can be promoted in the initial stage (eg, nucleation stage). This may be because, among other reasons, the local diffusion of the adsorbed Ti and N precursor molecules has more time to diffuse locally and wet the substrate surface (especially non-metallic surfaces) with a relatively low contact angle. TiN layers grown at relatively low exposure pressures result in layers that uniformly cover large areas of the non-metallic surface with virtually no formation of islands, making the initial growth phase more favorable to a layer-by-layer growth mode on the substrate surface , on the substrate surface, ALD TiN will generally favor the 3D island or SK growth modes as described above. Thus, by initiating ALD of TiN by exposing the substrate to Ti and/or N precursors at relatively low precursor exposure pressures (e.g., less than 3 Torr), the resulting initial layer can be grown in a layer-by-layer mode (e.g., during the nucleation stage). Subsequent bulk growth stages, which can be continued by exposing the substrate to Ti and/or N precursors at relatively high precursor exposure pressures (eg, greater than 3 Torr), can continue in a layer-by-layer mode. By using the method according to the embodiments, some disadvantages of the conventional ALD of TiN can be avoided, especially in inorganic layers of some semiconducting and/or insulating materials, including especially Si, SiO 2 and/or Si 3 N 4 , by ALD. ), this can generally be associated with initial growth characterized by island or SK growth modes as described above followed by columnar growth.

圖3A係示意性地繪示根據實施例之藉由使基板暴露至具有不同對應前驅體暴露壓力之複數個循環來形成TiN層之原子層沈積方法300的流程圖。所得膜可具有在不同對應暴露壓力下形成之至少兩個區域。圖3B示意性地繪示根據圖3A中所繪示之方法之包括藉由其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法形成之TiN層之半導體結構350的橫截面視圖。參考圖3A,方法300包含在經組態用於ALD (例如,熱ALD)之反應腔室中提供310包括非金屬表面之基板。此外,方法300包括初始階段(例如,成核階段),該初始階段包含藉由在第一各自暴露壓力下使半導體基板暴露至各包括至第一Ti前驅體及第一N前驅體之之暴露之一或多個第一ALD循環而在基板上形成320薄膜之第一部分。方法300進一步包括後期階段(例如,塊體沈積階段),包含藉由在第二各自暴露下使半導體基板暴露至各包括至第二Ti前驅體及第二N前驅體之暴露之一或多個第二ALD循環而在薄膜之第一部分上形成330薄膜之第二部分。相對於在該一或多個第一ALD循環期間至Ti前驅體及N前驅體之一或兩者之對應暴露,在該一或多個第二ALD循環期間至Ti前驅體及N前驅體之一或兩者之暴露係在較高壓力下。3A schematically depicts a flowchart of an atomic layer deposition method 300 for forming a TiN layer by exposing a substrate to a plurality of cycles with different corresponding precursor exposure pressures, according to an embodiment. The resulting film can have at least two regions formed at different corresponding exposure pressures. 3B schematically depicts a semiconductor structure 350 comprising a TiN layer formed by an atomic layer deposition method in which the substrate is exposed to a plurality of cycles with different corresponding precursor exposure pressures according to the method depicted in FIG. 3A Cross-sectional view. Referring to FIG. 3A , method 300 includes providing 310 a substrate including a non-metallic surface in a reaction chamber configured for ALD (eg, thermal ALD). Additionally, method 300 includes an initial phase (e.g., a nucleation phase) comprising exposing the semiconductor substrate to each of the first Ti precursor and the first N precursor by exposing the semiconductor substrate at a first respective exposure pressure. One or more first ALD cycles form 320 a first portion of the film on the substrate. The method 300 further includes a later stage (e.g., a bulk deposition stage) comprising exposing the semiconductor substrate to one or more of each including exposures to a second Ti precursor and a second N precursor under second respective exposures. A second ALD cycle forms 330 a second portion of the film on the first portion of the film. The exposure to the Ti precursor and the N precursor during the one or more second ALD cycles relative to the corresponding exposure to one or both of the Ti precursor and the N precursor during the one or more first ALD cycles Exposure to one or both is at higher pressures.

參考圖3B,包括基板360之半導體薄膜結構350之橫截面視圖,基板360繼而包括非金屬表面,例如,介電質及/或半導體表面。包括TiN之薄膜之第一部分370經形成於基板360上,且該薄膜之第二部分380經形成於第一部分370上。第一及第二部分370、380係藉由圖3A中所繪示之其中使基板360暴露至具有不同對應前驅體暴露壓力之第一及第二循環之原子層沈積方法來形成。由於第一部分370可在如上文所論述之初始階段(例如,成核階段)中以逐層生長模式生長,故至少第一部分370或第一及第二部分370、380兩者可實質上無藉由V形晶粒之柱狀生長及相對較高(例如,厚度之10%)表面粗糙度特性化之具有不同定向之相鄰晶體。相對於在成核及塊體沈積階段期間在單一壓力下形成之可比較薄膜層,所得TiN層具有包含相對較高保形性或階梯覆蓋率、較低表面粗糙度、較小平均晶粒大小、較高導電率及/或阻障特性之一或多者之優越性質。Referring to FIG. 3B , a cross-sectional view of a semiconductor thin film structure 350 including a substrate 360 , which in turn includes a non-metallic surface, eg, a dielectric and/or a semiconductor surface. A first portion 370 of a thin film comprising TiN is formed on the substrate 360 and a second portion 380 of the thin film is formed on the first portion 370 . The first and second portions 370, 380 are formed by the atomic layer deposition method depicted in FIG. 3A in which the substrate 360 is exposed to first and second cycles having different corresponding precursor exposure pressures. Since the first portion 370 can be grown in a layer-by-layer growth mode in an initial stage (e.g., a nucleation stage) as discussed above, at least the first portion 370 or both the first and second portions 370, 380 can be substantially free of defects. Neighboring crystals with different orientations characterized by columnar growth of V-shaped grains and relatively high (eg, 10% of thickness) surface roughness. Relative to comparable thin film layers formed under a single pressure during the nucleation and bulk deposition stages, the resulting TiN layer has properties including relatively higher conformality or step coverage, lower surface roughness, smaller average grain size, The superior properties of one or more of higher conductivity and/or barrier properties.

如在本文中及貫穿說明書所描述,將瞭解,其上形成根據實施例之TiN薄膜之半導體基板可以各種基板實施,包含(但不限於)可由以下形成之經摻雜半導體基板:IV族元素材料(例如,Si、Ge、C或Sn)或由IV族材料形成之合金(例如,SiGe、SiGeC、SiC、SiSn、SiSnC、GeSn等);III-V族化合物半導體材料(例如,GaAs、GaN、InAs等)或由III-V族材料形成之合金;II-VI族半導體材料(CdSe、CdS、ZnSe等)或由II-VI族材料形成之合金。As described herein and throughout the specification, it will be appreciated that semiconductor substrates on which TiN thin films according to embodiments are formed can be implemented with a variety of substrates, including but not limited to doped semiconductor substrates that can be formed from Group IV element materials (e.g., Si, Ge, C, or Sn) or alloys formed of group IV materials (e.g., SiGe, SiGeC, SiC, SiSn, SiSnC, GeSn, etc.); III-V group compound semiconductor materials (e.g., GaAs, GaN, InAs, etc.) or alloys formed by III-V materials; II-VI semiconductor materials (CdSe, CdS, ZnSe, etc.) or alloys formed by II-VI materials.

根據某些實施例,基板亦可實施為絕緣體上半導體,諸如絕緣體上矽(SOI)基板。SOI基板通常包含其中上文所描述之各種結構係使用諸如埋藏式SiO 2層之絕緣體層與支撐基板隔離之矽-絕緣體-矽結構。另外,將瞭解,本文中所描述之各種結構可至少部分形成於在表面區域處或附近形成之磊晶層中。 According to some embodiments, the substrate may also be implemented as a semiconductor-on-insulator, such as a silicon-on-insulator (SOI) substrate. SOI substrates typically include silicon-insulator-silicon structures in which the various structures described above are isolated from a supporting substrate using an insulator layer such as a buried SiO2 layer. Additionally, it will be appreciated that various structures described herein may be formed at least in part in an epitaxial layer formed at or near a surface region.

此外,基板可包含形成於其上之各種結構,僅舉幾例,例如,擴散區域、隔離區域、電極、通孔及線,可在其等上形成包括根據實施例之TiN層之任何結構,包含具有一或多個半導體或介電質表面之拓撲特徵(諸如通孔、腔、孔或溝渠)。因此,其上形成根據實施例之TiN層之非金屬表面可包含:半導體表面,例如,經摻雜或無摻雜之Si表面;及/或介電質表面,僅舉幾例,例如,層間介電質(ILD)表面、遮罩或硬遮罩表面或閘極介電質表面,其可包含無機絕緣體、氧化物、氮化物、高K介電質、低K介電質或碳,僅舉幾例介電材料。In addition, the substrate may include various structures formed thereon, such as diffusion regions, isolation regions, electrodes, vias, and lines, to name a few, on which any structure including the TiN layer according to the embodiment may be formed, Topological features (such as vias, cavities, holes or trenches) having one or more semiconductor or dielectric surfaces are included. Thus, non-metallic surfaces on which a TiN layer according to embodiments is formed may include: semiconductor surfaces, such as doped or undoped Si surfaces; and/or dielectric surfaces, such as interlayer Dielectric (ILD) surfaces, mask or hard mask surfaces, or gate dielectric surfaces, which may contain inorganic insulators, oxides, nitrides, high-K dielectrics, low-K dielectrics, or carbon, only A few examples of dielectric materials.

如在本文中及貫穿說明書所描述,反應器腔室係指包含單個晶圓處理反應腔室或批次晶圓處理反應腔室之適當地經組態用於熱原子層沈積(ALD)之任何反應腔室。在熱ALD反應器中,基板可放置於諸如基座或運搬艇(carrier boat)之合適基板固持器上。基板可藉由通過經加熱基座之傳導來直接加熱,或藉由來自輻射源(諸如燈)之輻射或藉由通過經加熱腔室壁之對流來間接加熱。As described herein and throughout the specification, a reactor chamber refers to any suitably configured for thermal atomic layer deposition (ALD), including a single wafer processing reaction chamber or a batch of wafer processing reaction chambers. reaction chamber. In a thermal ALD reactor, the substrate can be placed on a suitable substrate holder such as a susceptor or a carrier boat. The substrate can be heated directly by conduction through a heated susceptor, or indirectly by radiation from a radiation source, such as a lamp, or by convection through a heated chamber wall.

通常,在ALD程序中,將反應物或前驅體(例如,氧化及還原反應物)交替地引入至其中安置有基板之反應腔室中。一或多個反應物或前驅體之引入繼而可與用於自反應腔室移除過量反應物或前驅體之清除及/或抽出程序交替。可在適當時間段內在條件下將反應物引入至反應腔室中,使得用前驅體或反應物及/或反應物之反應產物使基板之表面變得至少部分飽和。接著可自基板移除過量或殘餘前驅體或反應物,諸如藉由清除及/或抽出反應腔室。可藉由合適真空泵抽程序來執行抽出程序且可藉由將非反應性或惰性氣體(例如,氮氣或稀有氣體)引入至反應腔室中來執行清除步驟。在下文實例中之藉由熱ALD形成之層之背景內容中,通常存在兩類前驅體或反應物,即,氮(N)前驅體及鈦(Ti)前驅體。Typically, in an ALD process, reactants or precursors (eg, oxidized and reduced reactants) are alternately introduced into a reaction chamber in which a substrate is disposed. The introduction of one or more reactants or precursors may then be alternated with purge and/or extraction procedures for removing excess reactants or precursors from the reaction chamber. The reactants may be introduced into the reaction chamber for a suitable period of time under conditions such that the surface of the substrate becomes at least partially saturated with the precursors or reactants and/or reaction products of the reactants. Excess or residual precursors or reactants can then be removed from the substrate, such as by purging and/or withdrawing the reaction chamber. The pumping procedure can be performed by a suitable vacuum pumping procedure and the purging step can be performed by introducing a non-reactive or inert gas, such as nitrogen or a noble gas, into the reaction chamber. In the context of layers formed by thermal ALD in the examples below, there are generally two types of precursors or reactants, nitrogen (N) precursors and titanium (Ti) precursors.

在下文中,參考圖4,根據實施例,藉由ALD (例如,熱ALD)形成具有藉由使基板暴露至具有不同對應前驅體暴露壓力之複數個循環來形成之至少兩個區域之包括TiN之薄膜之方法300 (圖3A)之實例性實施方案。 藉由使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之 TiN 之原子層沈積 In the following, referring to FIG. 4 , according to an embodiment, a layer comprising TiN having at least two regions formed by exposing the substrate to a plurality of cycles with different corresponding precursor exposure pressures is formed by ALD (eg, thermal ALD). An exemplary embodiment of a thin film method 300 (FIG. 3A). Atomic layer deposition of TiN by exposing substrates to multiple cycles with different corresponding precursor exposure pressures

再次參考圖3A,在反應腔室中提供310包括非金屬表面之基板(圖3B中之基板360)之後,方法300繼續藉由原子層沈積(ALD) (例如,熱ALD)憑藉使半導體基板暴露至一或多個第一ALD循環而在該非金屬表面上形成320薄膜之第一部分,接著藉由使半導體基板暴露至一或多個第二ALD循環而形成薄膜之第二部分。在下文中,用圖解法描述在該等第一及第二ALD循環期間施加之暴露壓力。Referring again to FIG. 3A , after providing 310 a substrate comprising a non-metallic surface (substrate 360 in FIG. 3B ) in a reaction chamber, the method 300 continues by exposing the semiconductor substrate by atomic layer deposition (ALD) (e.g., thermal ALD). A first portion of the film is formed 320 on the non-metallic surface to one or more first ALD cycles, followed by forming a second portion of the film by exposing the semiconductor substrate to one or more second ALD cycles. In the following, the exposure pressures applied during the first and second ALD cycles are described graphically.

圖4用圖解法繪示根據各項實施例之對應於在用於形成薄膜之第一部分370 (圖3B)之第一循環400A或階段(例如,成核階段)及用於形成薄膜之第二部分380 (圖3B)之第二循環400B或階段(例如,塊體生長階段)期間之基板至Ti及N前驅體之暴露的壓力跡線400。參考圖4,藉由使半導體基板暴露至各包括至第一Ti前驅體之分壓力之一或多次暴露404或暴露脈衝及至第一N前驅體之分壓力之一或多次暴露408或暴露脈衝之一或多個第一ALD循環400A來形成薄膜之第一部分。藉由使半導體基板暴露至各包括至第二Ti前驅體之分壓力之一或多次暴露412或暴露脈衝及至第二N前驅體之分壓力之一或多次暴露416或暴露脈衝之一或多個第二ALD循環400B來形成薄膜之第二部分。FIG. 4 diagrammatically depicts a first cycle 400A or stage (e.g., a nucleation stage) corresponding to a first portion 370 (FIG. 3B) for forming a thin film and a second cycle for forming a thin film, according to various embodiments. Pressure trace 400 of substrate to Ti and N precursor exposure during a second cycle 400B or phase (eg, bulk growth phase) of portion 380 (FIG. 3B). Referring to FIG. 4 , by exposing the semiconductor substrate to one or more exposures 404 or exposure pulses each comprising a partial pressure to the first Ti precursor and one or more exposures 408 or exposures to the first N precursor One or more first ALD cycles 400A are pulsed to form the first portion of the film. By exposing the semiconductor substrate to one or more exposures 412 or pulses of exposure each comprising a partial pressure to a second Ti precursor and one or more exposures 416 or pulses of exposure to a partial pressure to a second N precursor A plurality of second ALD cycles 400B are used to form the second portion of the thin film.

如示意性地描繪,至第一Ti前驅體之暴露404、至第一N前驅體之暴露408、至第二Ti前驅體之暴露412及至第二N前驅體之暴露416之各者可具有不同分壓力狀態(regime),包含對應分壓力上升狀態404A、408A、412A及416A、主暴露狀態404B、408B、412B及416B及分壓力下降狀態404C、408C、412C及416C。分壓力上升狀態404A、408A、412A及416A之各者可對應於(例如)引入至反應腔室中之各自前驅體。主暴露狀態404B、408B、412B及416B之各者可對應於在其間反應腔室中之各自前驅體之量相對恆定之週期。例如,可使用壓力傳感器或節流閥來維持各自前驅體之相對恆定量。分壓力下降狀態404C、408C、412C及416C之各者可對應於(例如)自反應腔室清除或抽出各自前驅體時之狀態。As schematically depicted, each of the exposure 404 to the first Ti precursor, the exposure 408 to the first N precursor, the exposure 412 to the second Ti precursor, and the exposure 416 to the second N precursor can have different Partial pressure regimes (regime) include corresponding partial pressure rise states 404A, 408A, 412A, and 416A, main exposure states 404B, 408B, 412B, and 416B, and partial pressure drop states 404C, 408C, 412C, and 416C. Each of the partial pressure rise states 404A, 408A, 412A, and 416A may correspond to, for example, a respective precursor introduced into the reaction chamber. Each of the main exposure states 404B, 408B, 412B, and 416B may correspond to a period during which the amount of the respective precursor in the reaction chamber is relatively constant. For example, pressure sensors or throttle valves can be used to maintain relatively constant amounts of the respective precursors. Each of the partial pressure drop states 404C, 408C, 412C, and 416C may correspond to, for example, the state when the respective precursors are purged or drawn from the reaction chamber.

仍參考圖4,將瞭解,在一些實施方案中,可在各次暴露之後抽出及/或清除前驅體。在其中可抽出而未清除前驅體之一些實施方案中,反應腔室壓力可實質上藉由各自前驅體之分壓力表示,且暴露404、408、412及416之壓力跡線可實質上表示在各自暴露期間之反應腔室壓力或前驅體分壓力。在其中用惰性氣體清除而未抽出前驅體之一些實施方案中,反應腔室壓力可藉由對應於暴露404、408、412及416之總反應腔室壓力404P、408P、412P及416P表示,其中該等總反應腔室壓力源自各自前驅體與惰性氣體之混合物。Still referring to FIG. 4 , it will be appreciated that, in some implementations, the precursor may be extracted and/or purged after each exposure. In some embodiments where the precursors can be drawn out without purging, the reaction chamber pressure can be represented substantially by the partial pressure of the respective precursors, and the pressure traces for exposures 404, 408, 412, and 416 can be represented substantially at Reaction chamber pressure or precursor partial pressure during the respective exposure periods. In some embodiments where the precursor is purged with an inert gas without evacuating the precursor, the reaction chamber pressure can be represented by the total reaction chamber pressures 404P, 408P, 412P, and 416P corresponding to exposures 404, 408, 412, and 416, where The total reaction chamber pressures are derived from the respective precursor and inert gas mixtures.

實際上,泵抽及清除之組合可用於較高處理量及改良之膜品質。在此等實施方案中,在量測包含清除及泵抽期間之總壓力404P、408P、412P及416P時,可使基板經受第一Ti前驅體、第一N前驅體、第二Ti前驅體及第二N前驅體之分壓力。在一些實施例中,在使用壓力傳感器並用惰性氣體代替經移除前驅體來調整泵抽功率時,可使總腔室壓力貫穿給定前驅體暴露或暴露脈衝保持相對恆定。在此等實施方案中,用於形成第一部分(圖3B中之370)之一或多個第一ALD循環400A各可包括至第一Ti前驅體之分壓力之一或多次暴露404 (在經量測參數可為總反應腔室壓力404P時),及至第一N前驅體之分壓力之一或多次暴露408 (在經量測參數可為總反應腔室壓力408P時)。類似地,用於形成第二部分(圖3B中之380)之一或多個第二ALD循環400B可各包括至第二Ti前驅體之分壓力之一或多次暴露412 (在經量測參數可為總壓力412P時),及至第二N前驅體之分壓力之一或多次暴露416 (在經量測參數可為總壓力416P時)。In fact, a combination of pumping and purging can be used for higher throughput and improved membrane quality. In these embodiments, the substrate may be subjected to a first Ti precursor, a first N precursor, a second Ti precursor, and Partial pressure of the second N precursor. In some embodiments, the total chamber pressure can be kept relatively constant throughout a given precursor exposure or exposure pulse while adjusting the pumping power using a pressure sensor and replacing the removed precursor with an inert gas. In such embodiments, each of the one or more first ALD cycles 400A used to form the first portion (370 in FIG. 3B ) may include one or more exposures 404 (at The measured parameter may be the total reaction chamber pressure 404P), and one or more exposures 408 to the partial pressure of the first N precursor (when the measured parameter may be the total reaction chamber pressure 408P). Similarly, one or more second ALD cycles 400B for forming the second portion (380 in FIG. 3B ) may each include one or more exposures 412 to the partial pressure of the second Ti precursor (after measured The parameter may be the total pressure 412P), and one or more exposures 416 to the partial pressure of the second N precursor (where the measured parameter may be the total pressure 416P).

根據各項實施例,在至前驅體之暴露期間,經量測之總反應腔室壓力可與該前驅體之分壓力成比例。因此,分別相對於總壓力404P及408P較高之總壓力412P及416P對應於第二Ti前驅體及第二N前驅體分別相對於第一Ti前驅體及第一N前驅體之分壓力較高之分壓力。然而,實施例並不限於此且在其他實施例中,分別相對於總壓力404P及408P較高之總壓力412P及416P可對應於第二Ti前驅體及第二N前驅體分別相對於第一Ti前驅體及第一N前驅體之分壓力相同或較低之分壓力。According to various embodiments, the measured total reaction chamber pressure may be proportional to the partial pressure of the precursor during exposure to the precursor. Thus, the higher total pressures 412P and 416P relative to the total pressures 404P and 408P, respectively, correspond to higher partial pressures of the second Ti precursor and the second N precursor relative to the first Ti precursor and the first N precursor, respectively. points of pressure. However, embodiments are not limited thereto and in other embodiments, higher total pressures 412P and 416P relative to total pressures 404P and 408P, respectively, may correspond to a second Ti precursor and a second N precursor relative to the first Partial pressures of the Ti precursor and the first N precursor are the same or lower.

再次參考圖3A中之所繪示方法300,相對於在初始(例如,成核階段)之一或多個第一ALD循環期間之第一Ti前驅體及第一N前驅體之暴露壓力之對應一或兩者,在後期階段(例如,塊體沈積階段)之一或多個第二ALD循環期間之第二Ti前驅體及第二N前驅體之暴露壓力之一或兩者係較高的。在一些實施例中,暴露壓力可為前驅體之分壓力或反應腔室之總壓力。因此,在各項實施例中,參考圖4,分別相對於至第一Ti前驅體之暴露404及至第一N前驅體之暴露408之對應一或兩者,至第二Ti前驅體之暴露412及至第二N前驅體之暴露416之一或兩者可在較高分壓力及/或較高總反應腔室壓力下。Referring again to the illustrated method 300 in FIG. 3A , the correspondence with respect to the exposure pressure of the first Ti precursor and the first N precursor during the initial (e.g., nucleation phase) one or more first ALD cycles One or both, one or both of the exposure pressures of the second Ti precursor and the second N precursor during one or more of the second ALD cycles at a later stage (e.g., bulk deposition stage) are higher . In some embodiments, the exposure pressure can be the partial pressure of the precursor or the total pressure of the reaction chamber. Thus, in various embodiments, referring to FIG. 4 , the exposure 412 to the second Ti precursor is relative to a corresponding one or both of the exposure 404 to the first Ti precursor and the exposure 408 to the first N precursor, respectively. Either or both of the exposure 416 to the second N precursor may be at a higher partial pressure and/or a higher total reaction chamber pressure.

仍參考圖4,在各項實施例中,在第一及第二循環400A及400B期間至Ti及N前驅體之對應暴露之間的對應分壓力或總壓力可為在分壓力上升狀態404A、408A、412A及416A、主暴露狀態404B、408B、412B及416B及分壓力下降狀態404C、408C、412C及416C之任一者期間之對應分壓力或總壓力。例如,相對於在第一ALD循環400A期間之分別在主暴露狀態404B及408B期間至第一Ti前驅體及第一N前驅體之一或兩者之暴露404、408,在第二ALD循環400B期間之分別在主暴露狀態412B及416B期間至第二Ti前驅體及第二N前驅體之一或兩者之暴露412、416可在較高總壓力或分壓力下。在各項其他實施例中,在第一及第二循環400A及400B期間至Ti及N前驅體之對應暴露之間的對應分壓力或總壓力可為在暴露404、408、412及416期間之對應平均值、平均數或峰值分壓力或總壓力。Still referring to FIG. 4 , in various embodiments, the corresponding partial or total pressures between the corresponding exposures to the Ti and N precursors during the first and second cycles 400A and 400B may be in the partial pressure rise state 404A, 408A, 412A, and 416A, the corresponding partial or total pressure during any of the main exposure states 404B, 408B, 412B, and 416B, and the partial pressure drop states 404C, 408C, 412C, and 416C. For example, relative to the exposures 404, 408 to one or both of the first Ti precursor and the first N precursor during the main exposure states 404B and 408B, respectively, during the first ALD cycle 400A, in the second ALD cycle 400B The exposures 412, 416 during the main exposure states 412B and 416B, respectively, to one or both of the second Ti precursor and the second N precursor may be at higher total or partial pressures. In various other embodiments, the corresponding partial or total pressures between the corresponding exposures to the Ti and N precursors during the first and second cycles 400A and 400B may be Corresponds to mean, mean or peak partial pressure or total pressure.

仍參考圖4,在所繪示實施例中,在至第一Ti前驅體之暴露404及至第一N前驅體之暴露408期間之總壓力及/或分壓力係不同的,且在至第二Ti前驅體之暴露412及至第二N前驅體之暴露416期間之總壓力及/或分壓力係不同的。然而,實施例並不限於此且在一些實施例中,在至第一Ti前驅體之暴露404及至第一N前驅體之暴露408期間之總壓力及/或分壓力可保持恆定,及/或在至第二Ti前驅體之暴露412及至第二N前驅體之暴露416期間之總壓力及/或分壓力可保持恆定。Still referring to FIG. 4 , in the illustrated embodiment, the total pressure and/or partial pressure during exposure 404 to the first Ti precursor and exposure 408 to the first N precursor are different, and during exposure to the second The total and/or partial pressures during the exposure 412 of the Ti precursor to the exposure 416 of the second N precursor are different. However, embodiments are not so limited and in some embodiments, the total pressure and/or partial pressure during the exposure 404 to the first Ti precursor and the exposure 408 to the first N precursor can be kept constant, and/or The total pressure and/or partial pressure during the exposure 412 to the second Ti precursor and the exposure 416 to the second N precursor can be kept constant.

仍參考圖4,在至第一Ti前驅體之暴露404及至第一N前驅體之暴露408期間之總壓力之各者(其可為相同或不同的)可為0.01托至0.2托、0.2托至0.4托、0.4托至0.6托、0.6托至0.8托、0.8托至1.0托、1.0托至1.5托、1.5托至2.0托、2.0托至2.5托、2.5托至3.0托或在藉由此等值之任一者界定之範圍內之壓力。在至第二Ti前驅體之暴露412及至第二N前驅體之暴露416期間之總壓力之各者(其可為相同或不同的)可為3.0托至4.0托、4.0托至5.0托、5.0托至6.0托、6.0托至7.0托、7.0托至8.0托、8.0托至9.0托、9.0托至10.0托、10.0托至11.0托、11.0托至12.0托或在藉由此等值之任一者界定之範圍內之壓力。在至第二Ti前驅體之暴露412及至第一Ti前驅體之暴露404期間之反應腔室之總壓力(以托為單位量測)之比率可為2至5、5至10、10至20、20至50、50至100,或在藉由此等值之任一者界定之範圍內。類似地,在至第二N前驅體之暴露416及至第一N前驅體之暴露408期間之反應腔室之總壓力之比率可為2至5、5至10、10至20、20至50、50至100,或在藉由此等值之任一者界定之範圍內。在暴露404、408、412及416之各者中,各自Ti或N前驅體可構成反應腔室中之氣體分子之總量之1%至2%、2%至5%、5%至10%、10%至20%、20%至50%、50%至100%,或在藉由此等值之任一者界定之範圍內之百分比。Still referring to FIG. 4 , each of the total pressure during the exposure 404 to the first Ti precursor and the exposure 408 to the first N precursor, which may be the same or different, may be 0.01 Torr to 0.2 Torr, 0.2 Torr to 0.4 Torr, 0.4 Torr to 0.6 Torr, 0.6 Torr to 0.8 Torr, 0.8 Torr to 1.0 Torr, 1.0 Torr to 1.5 Torr, 1.5 Torr to 2.0 Torr, 2.0 Torr to 2.5 Torr, 2.5 Torr to 3.0 Torr or by The pressure within the range defined by any one of the equivalent values. Each of the total pressure during exposure 412 to the second Ti precursor and exposure 416 to the second N precursor, which may be the same or different, may be 3.0 to 4.0 Torr, 4.0 to 5.0 Torr, 5.0 Torr to 6.0 Torr, 6.0 Torr to 7.0 Torr, 7.0 Torr to 8.0 Torr, 8.0 Torr to 9.0 Torr, 9.0 Torr to 10.0 Torr, 10.0 Torr to 11.0 Torr, 11.0 Torr to 12.0 Torr or any of these values The pressure within the defined range. The ratio of the total pressure of the reaction chamber (measured in Torr) during the exposure 412 to the second Ti precursor and the exposure 404 to the first Ti precursor can be 2 to 5, 5 to 10, 10 to 20 , 20 to 50, 50 to 100, or within a range defined by any of these values. Similarly, the ratio of the total pressure of the reaction chamber during the exposure 416 to the second N precursor and the exposure 408 to the first N precursor may be 2 to 5, 5 to 10, 10 to 20, 20 to 50, 50 to 100, or within the range defined by any of these values. In each of exposures 404, 408, 412, and 416, the respective Ti or N precursor may constitute 1% to 2%, 2% to 5%, 5% to 10% of the total amount of gas molecules in the reaction chamber , 10% to 20%, 20% to 50%, 50% to 100%, or a percentage within a range defined by any of these values.

仍參考圖4,根據各項實施例,控制在至第一Ti前驅體之暴露404及至第一N前驅體之暴露408期間之總壓力或分壓力,以及各自前驅體及惰性氣體之流動速率及反應腔室之泵抽功率,使得在第一循環400A或階段期間之沈積速率按包含至第一Ti前驅體之暴露404及至第一N前驅體之暴露408之每循環係0.10 Å/循環至0.20 Å/循環、0.20 Å/循環至0.30 Å/循環、0.30 Å/循環至0.40 Å/循環、0.40 Å/循環至0.50 Å/循環、0.50 Å/循環至0.60 Å/循環或在藉由此等值之任一者界定之範圍內之值。控制在至第二Ti前驅體之暴露412及至第二N前驅體之暴露416期間之總壓力或分壓力,以及各自前驅體及惰性氣體之流動速率及反應腔室之泵抽功率,使得在第二循環400B或階段期間之沈積速率按包含至第一Ti前驅體之暴露404及至第一N前驅體之暴露408之每循環係0.20 Å/循環至0.30 Å/循環、0.30 Å/循環至0.40 Å/循環、0.40 Å/循環至0.50 Å/循環、0.50 Å/循環至0.60 Å/循環、0.60 Å/循環至0.70 Å/循環、0.70 Å/循環至0.80 Å/循環或在藉由此等值之任一者界定之範圍內之值。在第二循環400B期間之每循環之沈積速率與在第一循環400A期間之每循環之沈積速率之比率可為1至1.5、1.5至2.0、2.5至3.0或在藉由此等值之任一者界定之範圍內之比率。Still referring to FIG. 4 , according to various embodiments, the total pressure or partial pressure during the exposure 404 to the first Ti precursor and the exposure 408 to the first N precursor, as well as the flow rates of the respective precursors and inert gases, and The pumping power of the reaction chamber is such that the deposition rate during the first cycle 400A or phase ranges from 0.10 Å/cycle to 0.20 Å/cycle per cycle comprising exposure 404 to the first Ti precursor and exposure 408 to the first N precursor. Å/cycle, 0.20 Å/cycle to 0.30 Å/cycle, 0.30 Å/cycle to 0.40 Å/cycle, 0.40 Å/cycle to 0.50 Å/cycle, 0.50 Å/cycle to 0.60 Å/cycle or by A value within the range defined by either of them. The total pressure or partial pressure during the exposure 412 to the second Ti precursor and the exposure 416 to the second N precursor, as well as the flow rates of the respective precursors and inert gases and the pumping power of the reaction chamber are controlled such that at The deposition rate during the second cycle 400B or stage is 0.20 Å/cycle to 0.30 Å/cycle, 0.30 Å/cycle to 0.40 Å per cycle comprising exposure 404 to the first Ti precursor and exposure 408 to the first N precursor /cycle, 0.40 Å/cycle to 0.50 Å/cycle, 0.50 Å/cycle to 0.60 Å/cycle, 0.60 Å/cycle to 0.70 Å/cycle, 0.70 Å/cycle to 0.80 Å/cycle, or between A value within the range defined by either. The ratio of the deposition rate per cycle during the second cycle 400B to the deposition rate per cycle during the first cycle 400A may be 1 to 1.5, 1.5 to 2.0, 2.5 to 3.0, or anywhere between such values. ratio within the range defined by the

本發明者已發現,當形成320 (圖3A)包括TiN之薄膜之第一部分370 (圖3B)及形成330 (圖3A)該薄膜之第二部分380 (圖3B)之各者包括使半導體基板分別暴露至第一循環400A (圖4)及第二循環400B (圖4)之1個至25個循環、26個至50個循環、50個至100個循環、100個至200個循環、200個至300個循環、300個至400個循環、400個至500個循環、500個至600個循環或在藉由此等值之任一者界定之範圍內之值時,可實現本文中所揭示之TiN薄膜之各種技術優點。根據各項實施例,第二循環之數目與第一循環之數目之比率可大於1、2、5或10或在藉由此等值之任一者界定之範圍內之比率,或小於1、0.5、0.1或在藉由此等值之任一者界定之範圍內之比率。包括TiN之包含第一部分370 (圖3B)及第二部分380 (圖3B)之薄膜之總厚度可具有不超過約25 nm、20 nm、15 nm、10 nm、7 nm、4 nm、2 nm或具有在藉由此等值之任一者界定之範圍內之值之經組合堆疊厚度。第一部分370 (圖3B)與第二部分380 (圖3B)之間的厚度比率可為約1:20至1:10、1:10至1:5、1:5至1:2、1:2至1:1、1:1至2:1、2:1至5:1、5:1至10:1、10:1至20:1或在藉由此等值之任一者界定之範圍內之比率。將瞭解,在一些實施例中,例如,當較高保形性相較於較低膜粗糙度可更重要時,第一部分370 (圖3B)可相對較薄,而在其他實施例中,例如,當較低膜粗糙度相較於較高保形性可更重要時,第二部分380 (圖3B)可相對較薄。The inventors have discovered that when each of forming 320 ( FIG. 3A ) a first portion 370 ( FIG. 3B ) of a thin film comprising TiN and forming 330 ( FIG. 3A ) a second portion 380 ( FIG. 3B ) of the thin film comprises making the semiconductor substrate 1 to 25 cycles, 26 to 50 cycles, 50 to 100 cycles, 100 to 200 cycles, 200 From 1 to 300 cycles, from 300 to 400 cycles, from 400 to 500 cycles, from 500 to 600 cycles, or at a value within the range defined by any of these values, the values described herein can be achieved Various technical advantages of the disclosed TiN thin films. According to various embodiments, the ratio of the number of second cycles to the number of first cycles may be greater than 1, 2, 5 or 10 or a ratio within a range defined by any of these values, or less than 1, 0.5, 0.1 or a ratio within a range defined by any of these values. The total thickness of the film comprising the first portion 370 ( FIG. 3B ) and the second portion 380 ( FIG. 3B ) including TiN may have a thickness of no more than about 25 nm, 20 nm, 15 nm, 10 nm, 7 nm, 4 nm, 2 nm or a combined stack thickness having a value within the range defined by any of these values. The thickness ratio between the first portion 370 (FIG. 3B) and the second portion 380 (FIG. 3B) may be about 1:20 to 1:10, 1:10 to 1:5, 1:5 to 1:2, 1:20 2 to 1:1, 1:1 to 2:1, 2:1 to 5:1, 5:1 to 10:1, 10:1 to 20:1 or defined by any of these values ratio within the range. It will be appreciated that in some embodiments, for example, when higher conformality may be more important than lower film roughness, first portion 370 ( FIG. 3B ) may be relatively thin, while in other embodiments, for example, When lower film roughness may be more important than higher conformality, second portion 380 (FIG. 3B) may be relatively thin.

仍參考圖4,基板至第一Ti前驅體之暴露404及基板至第二Ti前驅體之暴露412之各者係使得分別用第一Ti前驅體或第二Ti前驅體使基板之表面實質上或部分飽和。在基板至第一Ti前驅體之暴露404及基板至第二Ti前驅體之暴露412之各者之後,可抽出及/或清除未保持吸附或化學吸附於基板之表面上之過量或殘餘第一及/或第二Ti前驅體或其等之反應產物。Still referring to FIG. 4 , each of the exposure 404 of the substrate to the first Ti precursor and the exposure 412 of the substrate to the second Ti precursor is such that the surface of the substrate is substantially rendered substantially flat with the first Ti precursor or the second Ti precursor, respectively. or partially saturated. After each of the exposure 404 of the substrate to the first Ti precursor and the exposure 412 of the substrate to the second Ti precursor, excess or residual first Ti And/or the reaction product of the second Ti precursor or the like.

類似地,基板至第一N前驅體之暴露408及基板至第二N前驅體之暴露416之各者係使得分別用第一N前驅體或第二N前驅體使基板實質上或部分飽和。在基板至第一N前驅體之暴露408及基板至第二N前驅體之暴露416之各者之後,可抽出及/或清除未保持吸附或化學吸附於基板之表面上之過量或殘餘第一及/或第二N前驅體或其等之反應產物。使基板經受至第一Ti前驅體之一或多次暴露及至第一N前驅體之一或多次暴露可每TiN循環形成約一個單層或更少。類似地,使基板經受至第二Ti前驅體之一或多次暴露及至第二N前驅體之一或多次暴露可每TiN循環形成約一個單層或更少。Similarly, each of the exposure 408 of the substrate to the first N precursor and the exposure 416 of the substrate to the second N precursor is such that the substrate is substantially or partially saturated with the first N precursor or the second N precursor, respectively. After each of the exposure 408 of the substrate to the first N precursor and the exposure 416 of the substrate to the second N precursor, excess or residual first And/or the reaction product of the second N precursor or the like. Subjecting the substrate to one or more exposures to the first Ti precursor and one or more exposures to the first N precursor can form about one monolayer or less per TiN cycle. Similarly, subjecting the substrate to one or more exposures to a second Ti precursor and one or more exposures to a second N precursor can form about one monolayer or less per TiN cycle.

在一些實施例中,至第一Ti前驅體之暴露404、至第一N前驅體之暴露408、至第二Ti前驅體之暴露412及/或至第二N前驅體之暴露416可在其他前驅體之引入之前循序地執行複數次。例如,有利的是,在一些境況下,例如,在存在實質空間位阻效應時,使基板不止一次暴露至Ti前驅體及/或N前驅體可導致更高表面飽和位準。In some embodiments, the exposure 404 to the first Ti precursor, the exposure 408 to the first N precursor, the exposure 412 to the second Ti precursor, and/or the exposure 416 to the second N precursor may be at other The introduction of the precursor is performed sequentially multiple times. For example, it may be advantageous that exposing the substrate more than once to a Ti precursor and/or N precursor may result in higher surface saturation levels in some circumstances, eg, when substantial steric effects are present.

仍參考圖4,將瞭解,可取決於競爭情況選擇至第一Ti前驅體及至第一N前驅體之暴露之相對順序。在一些實施方案中,第一Ti前驅體有利地可為基板表面暴露至之第一前驅體。例如,Si表面至第一Ti前驅體之一或多次直接暴露可導致形成TiSi之一或多個單層且防止形成SiN,此繼而可有利於降低底層Si與形成於其上方之TiN層之間的接觸電阻。然而,在一些其他實施方案中,第一N前驅體有利地可為基板暴露至之第一前驅體。例如,藉由使Si基板直接暴露至第一N前驅體,可有意地形成SiN之一或多個單層,此可有利於改良堆疊之阻障特性。Still referring to FIG. 4 , it will be appreciated that the relative order of exposure to the first Ti precursor and to the first N precursor may be selected depending on competing conditions. In some embodiments, the first Ti precursor may advantageously be the first precursor to which the substrate surface is exposed. For example, one or more direct exposures of the Si surface to the first Ti precursor can result in the formation of one or more monolayers of TiSi and prevent the formation of SiN, which in turn can be beneficial in reducing the relationship between the underlying Si and the TiN layer formed above it. contact resistance between them. However, in some other embodiments, the first N precursor may advantageously be the first precursor to which the substrate is exposed. For example, by directly exposing the Si substrate to the first N precursor, one or more monolayers of SiN can be intentionally formed, which can be beneficial to improve the barrier properties of the stack.

將瞭解,在各項實施例中,基於包含對前驅體之空間位阻效應之易感性之各種考量,可改變在第一循環408A之各者中之基板至第一Ti反應物及/或第一N前驅體之暴露及在第二循環408B之各者中之至第二Ti反應物及/或第二N前驅體之暴露之頻率及重複率以獲得所要厚度及化學計量。It will be appreciated that in various embodiments, the substrate may be changed to the first Ti reactant and/or the second Ti reactant in each of the first cycles 408A based on various considerations including susceptibility to steric effects of the precursors. The frequency and repetition rate of the exposure of an N precursor and the exposure to the second Ti reactant and/or the second N precursor in each of the second cycles 408B to achieve the desired thickness and stoichiometry.

根據各項實施例,對於形成根據實施例之TiN層之第一及第二部分可為相同或不同之第一及第二Ti前驅體之非限制性實例包含四氯化鈦(TiCl 4)、四(二甲基胺基)鈦(TDMAT)或四(二乙基胺基)鈦(TDEAT)。對於TiN之第一及第二部分具有相同前驅體可為有利的,例如,成本較低及/或程序設計更容易。然而,例如,針對不同沈積特性或膜品質,對於TiN之第一及第二部分具有不同前驅體可為有利的。 According to various embodiments, non-limiting examples of first and second Ti precursors that may be the same or different for forming the first and second portions of the TiN layer according to embodiments include titanium tetrachloride (TiCl 4 ), Tetrakis(dimethylamino)titanium (TDMAT) or tetrakis(diethylamido)titanium (TDEAT). It may be advantageous to have the same precursor for the first and second portions of TiN, eg, lower cost and/or easier programming. However, it may be advantageous to have different precursors for the first and second portions of TiN, eg for different deposition characteristics or film qualities.

根據各項實施例,對於形成根據實施例之TiN層之第一及第二部分可為相同或不同之第一及第二N前驅體之非限制性實例包含氨(NH 3)、聯氨(N 2H 4)或甲基聯氨(CH 3(NH)NH 2、「MMH」)。對於TiN之第一及第二部分具有相同前驅體可為有利的,例如,成本較低及/或程序設計更容易。然而,例如,針對不同沈積特性或膜品質,對於TiN之第一及第二部分具有不同前驅體可為有利的。 According to various embodiments, non-limiting examples of first and second N precursors that may be the same or different for forming the first and second portions of the TiN layer according to embodiments include ammonia (NH 3 ), hydrazine ( N 2 H 4 ) or methylhydrazine (CH 3 (NH)NH 2 , “MMH”). It may be advantageous to have the same precursor for the first and second portions of TiN, eg, lower cost and/or easier programming. However, it may be advantageous to have different precursors for the first and second portions of TiN, eg for different deposition characteristics or film qualities.

根據各項實施例,用於清除之惰性氣體之非限制性實例可包含氮氣N 2或稀有氣體(諸如Ar或He)。 According to various embodiments, non-limiting examples of inert gases used for purge may include nitrogen N 2 or noble gases such as Ar or He.

根據實施例,當在350 oC至800 oC、450 oC至750 oC、500 oC至700 oC、550 oC至650 oC或在藉由此等值之任一者界定之範圍內(例如,約600 oC)之基板溫度下形成包括TiN之薄膜之第一部分370及第二部分380 (圖3B)之一或兩者時,可實現本文中所描述之各種技術優點及益處。在第一部分370及第二部分380之生長期間使溫度保持相同可有利於處理量並易於程序控制,因為在程序期間之溫度調整可能需要很長時間。 According to an embodiment, when at 350 ° C to 800 ° C, 450 ° C to 750 ° C, 500 ° C to 700 ° C, 550 ° C to 650 ° C or defined by any one of these values When one or both of the first portion 370 and the second portion 380 ( FIG. 3B ) comprising a thin film of TiN are formed at substrate temperatures in the range (e.g., about 600 ° C.), various technical advantages and advantages described herein can be realized. benefit. Keeping the temperature the same during the growth of the first portion 370 and the second portion 380 can be beneficial for throughput and ease of program control since temperature adjustments during the process can take a long time.

在各項實施例中,第一及第二Ti前驅體以及第一及第二N前驅體之各者之暴露時間或脈衝時間可在約0.1秒至1秒、1秒至10秒、10秒至30秒、30秒至60秒之範圍內,或可為藉由此等值之任一者界定之範圍內之持續時間。In various embodiments, the exposure time or pulse time of each of the first and second Ti precursors and the first and second N precursors can be in the range of about 0.1 seconds to 1 second, 1 second to 10 seconds, 10 seconds to 30 seconds, 30 seconds to 60 seconds, or may be a duration within a range defined by any of these values.

有利的是,當使用根據各項實施例之其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法來形成TiN層時,可將表面粗糙度及電阻率之一或兩者實質上降低至包含使用具有單個壓力設定點之其他ALD程序形成之TiN膜之習知TiN膜。在經沈積時,根據本文中所描述之方法形成且具有上述厚度及第一部分370與第二部分380 (圖3B)之間的厚度比率之包括TiN之薄膜可具有在薄膜之平均厚度之基礎上之3%、4%、5%、6%、7%、8%及9%或在藉由此等值之任一者界定之範圍內之值之均方根(RMS)表面粗糙度。替代性地,在經沈積時,具有上述厚度及第一部分370與第二部分380 (圖3B)之間的厚度比率之包括TiN之薄膜可具有小於2.5 nm、2 nm、1.5 nm、1.0 nm、0.5 nm或在藉由此等值之任一者界定之範圍內之值之RMS表面粗糙度值。Advantageously, when forming the TiN layer using an atomic layer deposition method according to various embodiments in which the substrate is exposed to a plurality of cycles with different corresponding precursor exposure pressures, one of surface roughness and resistivity or Both are substantially reduced to conventional TiN films comprising TiN films formed using other ALD procedures with a single pressure set point. When deposited, a thin film comprising TiN formed according to the methods described herein and having the thicknesses described above and the thickness ratio between the first portion 370 and the second portion 380 ( FIG. 3B ) can have a thickness based on the average thickness of the film. Root mean square (RMS) surface roughness of 3%, 4%, 5%, 6%, 7%, 8% and 9% or a value within the range defined by any of these values. Alternatively, a thin film comprising TiN having the aforementioned thickness and thickness ratio between the first portion 370 and the second portion 380 ( FIG. 3B ) may have a thickness of less than 2.5 nm, 2 nm, 1.5 nm, 1.0 nm, RMS surface roughness value of 0.5 nm or a value within the range defined by any of these values.

在經沈積時,根據本文中所描述之方法形成且具有上述厚度及第一部分370與第二部分380 (圖3B)之間的厚度比率之包括TiN之薄膜可具有<70 μΩ-cm、70 μΩ-cm至100 μΩ-cm、100 μΩ-cm至130 μΩ-cm、130 μΩ-cm至160 μΩ-cm、160 μΩ-cm至190 μΩ-cm、190 μΩ-cm至220 μΩ-cm、220 μΩ-cm至250 μΩ-cm、250 μΩ-cm至280 μΩ-cm、280 μΩ-cm至310 μΩ-cm或大於310 μΩ-cm,或在藉由此等值之任一者界定之範圍內(例如,小於約200 μΩ-cm)之值之電阻率。When deposited, a thin film comprising TiN formed according to the methods described herein and having the aforementioned thicknesses and thickness ratios between first portion 370 and second portion 380 ( FIG. 3B ) can have <70 μΩ-cm, 70 μΩ -cm to 100 μΩ-cm, 100 μΩ-cm to 130 μΩ-cm, 130 μΩ-cm to 160 μΩ-cm, 160 μΩ-cm to 190 μΩ-cm, 190 μΩ-cm to 220 μΩ-cm, 220 μΩ -cm to 250 μΩ-cm, 250 μΩ-cm to 280 μΩ-cm, 280 μΩ-cm to 310 μΩ-cm, or greater than 310 μΩ-cm, or within a range defined by any of these values ( For example, a resistivity of a value less than about 200 μΩ-cm).

除了降低表面粗糙度及電阻率之外,根據本文中所揭示之方法形成之包括TiN之薄膜在沈積於高縱橫比結構中時亦具有高保形性。在高縱橫比結構之背景內容中,保形性之一量度在本文中被稱為階梯覆蓋率。例如,高縱橫比結構可為通孔、孔、溝渠、腔或類似結構。藉由闡釋性實例,圖5示意性地繪示具有形成於其中之實例性高縱橫比結構516之半導體結構500,以繪示定義及/或量測形成於高縱橫比結構上之薄膜之保形性之一些實例性度量。所繪示之高縱橫比結構516係用在其之不同部分處具有不同厚度之TiN層512加襯裡。如本文中所描述,高縱橫比結構具有超過1之縱橫比,例如,定義為高縱橫比結構516之深度或高度(H)除以開口區域處之寬度(W)之比率。在所繪示實例中,高縱橫比結構516係經形成穿過形成於半導體基板504上之介電質層508 (例如,層間介電質(ILD)層)之通孔,使得高縱橫比結構516之底表面暴露底層半導體504。TiN層512可以不同厚度塗佈高縱橫比結構516之不同表面。如本文中所描述,用於定義或量測以高縱橫比形成之薄膜之保形性之一個度量被稱為階梯覆蓋率。階梯覆蓋率可定義為薄膜在高縱橫比結構之下或底部區域處之厚度與該薄膜在該高縱橫比結構之上或頂部區域處之厚度之間的比率。該上或頂部區域可為高縱橫比結構之在相對較小深度處(例如,在自開口之頂部量測之H之0至10%或0至25%處)之區域。該下或底部區域可為高縱橫比結構之在相對較大深度處(例如,在自開口之頂部量測之H之90%至100%或75%至100%處)之區域。在一些高縱橫比結構中,可藉由形成於高縱橫比結構之底表面處之薄膜512A之厚度與形成於高縱橫比結構之上或頂部側壁表面處之薄膜512C之厚度之比率來定義或量測階梯覆蓋率。然而,將瞭解,一些高縱橫比結構可能不具有明確定義之底表面或具有小曲率半徑之底表面。在此等結構中,可藉由形成於高縱橫比結構之下或底部側壁表面處之薄膜512B之厚度與形成於高縱橫比結構之上或頂部側壁表面處之薄膜512C之厚度之比率來更一致地定義或量測階梯覆蓋率。In addition to reducing surface roughness and resistivity, thin films comprising TiN formed according to the methods disclosed herein are also highly conformal when deposited in high aspect ratio structures. In the context of high aspect ratio structures, one measure of conformality is referred to herein as step coverage. For example, the high aspect ratio structures may be vias, holes, trenches, cavities, or similar structures. By way of illustrative example, FIG. 5 schematically depicts a semiconductor structure 500 having an example high aspect ratio structure 516 formed therein to illustrate defining and/or measuring the retention of thin films formed on the high aspect ratio structure. Some example measures of formality. The depicted high aspect ratio structure 516 is lined with a TiN layer 512 having different thicknesses at different portions thereof. As described herein, a high aspect ratio structure has an aspect ratio exceeding 1, eg, defined as the ratio of the depth or height (H) of the high aspect ratio structure 516 divided by the width (W) at the open area. In the depicted example, the high aspect ratio structure 516 is formed via a via through a dielectric layer 508 (eg, an interlayer dielectric (ILD) layer) formed on the semiconductor substrate 504 such that the high aspect ratio structure The bottom surface of 516 exposes the underlying semiconductor 504 . The TiN layer 512 can coat different surfaces of the high aspect ratio structure 516 with different thicknesses. As described herein, one metric used to define or measure the conformality of films formed at high aspect ratios is called step coverage. Step coverage can be defined as the ratio between the thickness of a film below or at the bottom region of a high aspect ratio structure and the thickness of the film above or at the top region of the high aspect ratio structure. The upper or top region may be a region of the high aspect ratio structure at a relatively small depth (eg, at 0 to 10% or 0 to 25% of H measured from the top of the opening). The lower or bottom region may be the region of the high aspect ratio structure at a relatively greater depth (eg, at 90% to 100% or 75% to 100% of H measured from the top of the opening). In some high aspect ratio structures, it may be defined by the ratio of the thickness of film 512A formed at the bottom surface of the high aspect ratio structure to the thickness of film 512C formed above or at the top sidewall surface of the high aspect ratio structure or Measure ladder coverage. However, it will be appreciated that some high aspect ratio structures may not have a well-defined bottom surface or have a bottom surface with a small radius of curvature. In such structures, the ratio of the thickness of the film 512B formed under the high aspect ratio structure or at the bottom sidewall surface to the thickness of the film 512C formed above the high aspect ratio structure or at the top sidewall surface can be adjusted. Consistently define or measure ladder coverage.

如上文所描述,根據本文中所揭示之方法形成之包括TiN之薄膜導致降低之表面粗糙度及電阻率,同時亦在高縱橫比結構中提供高保形性。根據各項實施例,可根據實施例以如本文中所定義之超過70%、80%、90%、95%或具有在藉由此等值之任一者界定之範圍內之值之階梯覆蓋率用TiN膜保形地塗佈具有超過1、2、5、10、20、50、100、200或在藉由此等值之任一者界定之範圍內之值之縱橫比之高縱橫比結構。 藉由使基板暴露至具有不同對應前驅體暴露壓力之複數個循環而形成之 TiN 之實體特性化 As described above, thin films comprising TiN formed according to the methods disclosed herein result in reduced surface roughness and resistivity, while also providing high conformality in high aspect ratio structures. According to various embodiments, it may be covered in steps exceeding 70%, 80%, 90%, 95% as defined herein, or having a value within a range defined by any of these values, according to embodiments Conformally coating with a TiN film has a high aspect ratio of an aspect ratio exceeding 1, 2, 5, 10, 20, 50, 100, 200, or a value within a range defined by any of these values structure. Physical characterization of TiN formed by exposing substrates to multiple cycles with different corresponding precursor exposure pressures

圖6係繪示在0.5托之相對較低腔室壓力下在總計600個經組合第一循環(例如,成核階段)及第二循環(例如,塊體沈積階段)中依據至Ti及N前驅體之暴露之第一循環之數目而變化之實驗量測之均方根(RMS)表面粗糙度趨勢604及階梯覆蓋率趨勢608。至Ti及N前驅體之暴露之第二循環係在5托之相對較高腔室壓力下。圖6中之各實驗資料點係自用於表面粗糙度量測之生長於經SiO 2塗佈之原生Si基板上之TiN膜及生長於形成於SiO 2中且具有約40:1縱橫比之通孔中之TiN膜獲取。第一及第二循環之經量測沈積速率分別係0.28 Å/循環及0.38 Å/循環。實驗資料係在用0個第一循環(0 Å) / 600個第二循環(228 Å)、50個第一循環(14 Å) / 550個第二循環(209 Å)、200個第一循環(56 Å) / 400個第二循環(152 Å)及600個第一循環(168 Å) / 0個第二循環(0 Å)生長之四個不同TiN膜上量測。該四個TiN膜分別具有約228 Å、223 Å、208 Å及168 Å之總厚度。如上文所描述,TiN膜之經量測表面粗糙度值隨著包含在相對較低壓力下之暴露之第一循環之相對數目增加而減小。在不受任何理論約束之情況下,此可係因為較低生長速率傾向於容許更多表面擴散,此傾向於降低表面粗糙度並促進逐層生長。用於以0個第一循環/ 600個第二循環、50個第一循環/ 550個第二循環及200個第一循環/ 400個第二循環生長之薄膜之經量測表面粗糙度值分別為約21 Å、17.5 Å及12.5 Å,對應於在各自TiN膜之總厚度之基礎上之約9%、8%及6%。另外,如上文所論述,相對於用600個第一循環/ 0個第二循環生長之膜,對於用0個第一循環/ 600個第二循環生長之薄膜,TiN膜之經量測階梯覆蓋率值更高。在不受任何理論約束之情況下,此可係因為較高壓力傾向於容許更多前驅體到達高縱橫比通孔之底部,此傾向於改良階梯覆蓋率。然而,令人驚訝的是,本發明者已發現,直至約50個第一循環(循環總數之8%),第一循環之增加數目實際上改良階梯覆蓋率。因此,根據一些實施例中,形成TiN膜之第一部分包括使半導體基板交替地暴露至各包括在小於約3托之相對較低暴露壓力下至第一Ti前驅體之暴露及至第一N前驅體之暴露之1個至50個循環。 FIG. 6 is a graph showing a total of 600 combined first cycles (e.g., nucleation phase) and second cycles (e.g., bulk deposition phase) to Ti and N at a relatively low chamber pressure of 0.5 Torr. The experimentally measured root mean square (RMS) surface roughness trend 604 and step coverage trend 608 as a function of the number of first cycles of exposure of the precursor. The second cycle of exposure to Ti and N precursors was at a relatively high chamber pressure of 5 Torr. The experimental data points in Fig. 6 were obtained from TiN films grown on SiO2 -coated native Si substrates and TiN films formed in SiO2 with an aspect ratio of about 40:1 for surface roughness measurements. The TiN film in the hole is obtained. The measured deposition rates for the first and second cycles were 0.28 Å/cycle and 0.38 Å/cycle, respectively. The experimental data is based on 0 first cycle (0 Å) / 600 second cycle (228 Å), 50 first cycle (14 Å) / 550 second cycle (209 Å), 200 first cycle (56 Å) / 400 second cycles (152 Å) and 600 first cycles (168 Å) / 0 second cycles (0 Å) on four different TiN films grown. The four TiN films have total thicknesses of about 228 Å, 223 Å, 208 Å, and 168 Å, respectively. As described above, the measured surface roughness values of the TiN films decreased as the relative number of first cycles comprising exposure at relatively lower pressures increased. Without being bound by any theory, this may be because lower growth rates tend to allow more surface diffusion, which tends to reduce surface roughness and promote layer-by-layer growth. Measured surface roughness values for films grown with 0 first cycle/600 second cycle, 50 first cycle/550 second cycle, and 200 first cycle/400 second cycle, respectively are about 21 Å, 17.5 Å and 12.5 Å, corresponding to about 9%, 8% and 6% on the basis of the total thickness of the respective TiN films. In addition, as discussed above, the measured step coverage of the TiN film for the film grown with 0 first cycle/600 second cycle relative to the film grown with 600 first cycle/0 second cycle Rate value is higher. Without being bound by any theory, this may be because higher pressure tends to allow more precursor to reach the bottom of the high aspect ratio via, which tends to improve step coverage. Surprisingly, however, the inventors have found that up to about 50 first cycles (8% of the total number of cycles), increasing the number of first cycles actually improves step coverage. Thus, according to some embodiments, forming the first portion of the TiN film includes alternately exposing the semiconductor substrate to a first Ti precursor and to a first N precursor each at a relatively low exposure pressure of less than about 3 Torr. 1 to 50 cycles of exposure.

圖7A至圖9繪示根據實施例之在藉由使基板暴露至具有相同前驅體暴露壓力之循環而生長之TiN膜與藉由使基板暴露至具有不同對應前驅體暴露壓力之複數個循環而生長之TiN膜之間的進一步實驗比較。圖7A係用藉由其中在對應於第二循環之相同前驅體暴露壓力下使基板暴露至ALD循環之原子層沈積方法形成之TiN層加襯裡之高縱橫比通孔的橫截面透射電子顯微照片。圖7B及圖7C係僅使用在5托之相對較高腔室壓力下至Ti及N前驅體之暴露之第二循環來生長之TiN膜的透射電子顯微照片(TEM)。該等TEM係在形成於SiO 2中之具有約40:1縱橫比之通孔之上(圖7B)區域及下(圖7C)區域處獲取之該通孔之影像。相比而言,圖8A及圖8B係根據實施例之使用在相對較低(0.5托)及較高(5托)腔室壓力下至Ti及N前驅體之暴露之第一及第二循環之組合來生長之TiN膜的透射電子顯微照片(TEM)。該等TEM係在形成於SiO 2中之具有約40:1縱橫比之通孔之上(圖8A)區域及下(圖8B)區域處獲取之該通孔之影像。圖9係繪示在自展示於圖7A至圖7C中之TEM顯微照片量測之經量測階梯覆蓋率904與自展示於圖8A至圖8B中之TEM顯微照片量測之經量測階梯覆蓋率908之間的實驗統計比較的圖表。圖9中之資料點表示自通孔之下區域內之不同位置及通孔之上區域內之不同位置獲取之比率。雖然自TEM影像不容易看出,但圖9中之統計比較清楚地繪示根據實施例沈積之TiN膜之93%之較高中值階梯覆蓋率及使用單一暴露壓力沈積之TiN膜之87%之中值階梯覆蓋率。另外,根據實施例沈積之TiN膜之經量測階梯覆蓋率之統計分佈係實質上小於使用單一暴露壓力沈積之TiN膜之經量測階梯覆蓋率之統計分佈,從而指示後者之膜粗糙度顯著更高。 具有增加之 (111) 結晶紋理之 TiN 薄膜之原子層沈積 7A-9 illustrate the growth of TiN films grown by exposing substrates to cycles with the same precursor exposure pressure and by exposing the substrate to a plurality of cycles with different corresponding precursor exposure pressures, according to embodiments. Further experimental comparison between as-grown TiN films. 7A is a cross-sectional transmission electron microscope of a TiN layer lined high aspect ratio via formed by an atomic layer deposition method in which the substrate is exposed to an ALD cycle at the same precursor exposure pressure corresponding to the second cycle. photo. 7B and 7C are transmission electron micrographs (TEM) of TiN films grown using only the second cycle of exposure to Ti and N precursors at a relatively high chamber pressure of 5 Torr. The TEM images were taken at regions above ( FIG. 7B ) and below ( FIG. 7C ) the via formed in SiO 2 with an aspect ratio of about 40:1. In contrast, FIGS. 8A and 8B are first and second cycles of exposure to Ti and N precursors using relatively low (0.5 Torr) and high (5 Torr) chamber pressures, according to embodiments. Transmission electron micrographs (TEM) of TiN films grown in combination with . The TEM images were taken at regions above (FIG. 8A) and below (FIG. 8B) the via formed in SiO2 with an aspect ratio of about 40:1. FIG. 9 is a graph showing the measured step coverage 904 measured from the TEM micrographs shown in FIGS. 7A-7C and measured from the TEM micrographs shown in FIGS. 8A-8B A graph of experimental statistical comparisons between measured ladder coverage 908. The data points in FIG. 9 represent ratios taken from different locations in the area below the via and different locations in the area above the via. Although not readily apparent from the TEM images, the statistics in Figure 9 more clearly show the higher median step coverage of 93% for the TiN film deposited according to the examples and 87% for the TiN film deposited using a single exposure pressure. Median ladder coverage. In addition, the statistical distribution of measured step coverage for TiN films deposited according to the examples was substantially smaller than the statistical distribution of measured step coverage for TiN films deposited using a single exposure pressure, indicating that the film roughness of the latter is significant higher. Atomic Layer Deposition of TiN Thin Films with Increased (111) Crystal Texture

對於TiN薄膜之特定應用(例如,DRAM電容器電極),為滿足日益增長之積極按比例調整的需求,TiN膜可能需要非常薄(例如,少於30 nm),而同時滿足嚴格電及機械性質之組合。例如,除了如上文所論述之低電阻率及高保形性之外,亦需要一些TiN薄膜同時滿足嚴格機械性質(例如,相對較高密度、硬度及模量)之組合,以便減少整合失敗之風險。For specific applications of TiN thin films (e.g., DRAM capacitor electrodes), to meet the increasing demand for positive scaling, TiN films may need to be very thin (e.g., less than 30 nm) while meeting stringent requirements for electrical and mechanical properties. combination. For example, in addition to low resistivity and high conformality as discussed above, some TiN films are also required to simultaneously satisfy a combination of stringent mechanical properties (e.g., relatively high density, hardness, and modulus) in order to reduce the risk of integration failure .

藉由原子層沈積生長之TiN膜可具有擁有包含表面處之(111)及(200)定向以及其他定向之不同晶向之晶粒。本發明者已發現,經紋理化以具有特定結晶紋理之TiN薄膜除了具有如上文所描述之所要低電阻率及保形性之外亦可具有優越機械性質。特定言之,具有相對較高(111)結晶紋理之超薄TiN膜可具有相對較高密度、硬度及模量。另外,增加之(111)結晶紋理可減少柱狀生長,從而提供優越擴散阻障性質。不欲受任何理論約束,具有相對較高(111)結晶紋理之TiN薄膜之此等有利性質可與在平行於生長表面之方向上之最高表面原子堆積密度以及有利於優越實體性質之晶粒邊界配置之一者相關聯。本發明者已進一步發現,如本文中所描述,可藉由控制週期性氣相沈積循環之特定條件來控制TiN薄膜之紋理。特定言之,本發明者已發現,其中使基板經受N前驅體之相對較高流動速率之週期性氣相沈積循環可引起TiN薄膜以相對較高(111)結晶紋理生長,如本文中所描述。TiN films grown by atomic layer deposition can have grains with different crystallographic orientations including (111) and (200) orientations at the surface, as well as other orientations. The inventors have discovered that TiN thin films textured to have a specific crystalline texture can have superior mechanical properties in addition to the desired low resistivity and conformality as described above. In particular, ultrathin TiN films with relatively high (111) crystalline texture can have relatively high density, hardness and modulus. In addition, the increased (111) crystalline texture can reduce columnar growth, thereby providing superior diffusion barrier properties. Without wishing to be bound by any theory, these favorable properties of TiN thin films with relatively high (111) crystalline texture can be related to the highest surface atomic packing density in the direction parallel to the growth surface and the grain boundaries that favor superior bulk properties. One of the configurations is associated. The present inventors have further discovered that, as described herein, the texture of TiN thin films can be controlled by controlling the specific conditions of the periodic vapor deposition cycles. In particular, the inventors have discovered that periodic vapor deposition cycles in which the substrate is subjected to a relatively high flow rate of N precursor can cause TiN thin films to grow with a relatively high (111) crystalline texture, as described herein .

圖11係示意性地繪示根據實施例之藉由使基板暴露至相對較高N前驅體流動速率而形成具有相對較高(111)結晶紋理之TiN層之原子層沈積方法1100的流程圖。方法1100包含提供1110半導體基板。此外,方法1100包含使該半導體基板暴露1120至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環。方法1100藉由使半導體基板暴露1120至其中N前驅體流動速率與Ti前驅體流動速率之比率(N/Ti流量比)及/或N前驅體之流動速率相較於習知方法實質上為高之一或多個週期性氣相沈積循環而形成具有相對較高(111)結晶紋理之TiN膜。根據各項實施例,N前驅體流動速率與Ti前驅體流動速率之比率(N/Ti流量比)超過3。根據各項實施例,N前驅體流動速率超過500 sccm。將瞭解,暴露1120及形成1130不一定如所展示般排序。本文中描述方法1100之各項實施方案。11 schematically depicts a flowchart of an atomic layer deposition method 1100 for forming a TiN layer with a relatively high (111) crystalline texture by exposing a substrate to a relatively high N precursor flow rate, according to an embodiment. Method 1100 includes providing 1110 a semiconductor substrate. Additionally, the method 1100 includes exposing 1120 the semiconductor substrate to one or more periodic vapor deposition cycles each comprising exposure to the Ti precursor at the Ti precursor flow rate and exposure to the N precursor at the N precursor flow rate. . Method 1100 operates by exposing 1120 a semiconductor substrate to which the ratio of N precursor flow rate to Ti precursor flow rate (N/Ti flow ratio) and/or the flow rate of N precursor is substantially higher than conventional methods One or more periodic vapor deposition cycles form a TiN film with a relatively high (111) crystalline texture. According to various embodiments, the ratio of N precursor flow rate to Ti precursor flow rate (N/Ti flow ratio) exceeds 3. According to various embodiments, the N precursor flow rate exceeds 500 sccm. It will be appreciated that exposing 1120 and forming 1130 are not necessarily ordered as shown. Various implementations of the method 1100 are described herein.

提供1110半導體基板可類似於根據上文關於圖3A及圖3B所描述之各項實施例提供310半導體基板,為簡潔起見,在本文中不重複其細節。例如,基板可經圖案化或未圖案化,且可具有如上文所描述之絕緣及導電表面之一或兩者。Providing 1110 the semiconductor substrate may be similar to providing 310 the semiconductor substrate according to the various embodiments described above with respect to FIGS. 3A and 3B , details of which are not repeated herein for the sake of brevity. For example, the substrate may be patterned or unpatterned, and may have one or both of insulating and conductive surfaces as described above.

使半導體基板暴露1120可類似於如上文關於圖3A、圖3B及圖4所描述之使半導體基板暴露至一或多個第一或第二熱ALD循環,為簡潔起見,在本文中不重複其細節。例如,以Ti前驅體流動速率至Ti前驅體之暴露可根據至第一Ti前驅體之暴露404 (圖4)或至第二Ti前驅體之暴露412 (圖4)。類似地,以N前驅體流動速率至N前驅體之暴露可根據至第一N前驅體之暴露408 (圖4)或至第二N前驅體之暴露416 (圖4)。為簡潔起見,在本文中不重複此等程序之細節。根據各項實施例,暴露1120使得形成具有高(111)結晶紋理之TiN薄膜,如本文中所描述。Exposing 1120 the semiconductor substrate may be similar to exposing the semiconductor substrate to one or more first or second thermal ALD cycles as described above with respect to FIGS. 3A , 3B and 4 and is not repeated here for brevity. its details. For example, the exposure to the Ti precursor at the Ti precursor flow rate may be based on the exposure 404 (FIG. 4) to the first Ti precursor or the exposure 412 (FIG. 4) to the second Ti precursor. Similarly, the exposure to the N precursor at the N precursor flow rate may be in accordance with the exposure 408 (FIG. 4) to the first N precursor or the exposure 416 (FIG. 4) to the second N precursor. For brevity, the details of these procedures are not repeated herein. According to various embodiments, exposing 1120 results in the formation of a TiN film with a high (111) crystalline texture, as described herein.

根據各項實施例,Ti前驅體及N前驅體可為上文所描述之前驅體之任一者。例如,Ti前驅體可為四氯化鈦(TiCl 4)且N前驅體可為氨(NH 3)。 According to various embodiments, the Ti precursor and the N precursor may be any of the precursors described above. For example, the Ti precursor may be titanium tetrachloride (TiCl 4 ) and the N precursor may be ammonia (NH 3 ).

包含基板溫度、腔室壓力及暴露時間之各種其他程序參數可根據上文所描述之各種程序參數,為簡潔起見,在本文中不重複其細節。Various other process parameters including substrate temperature, chamber pressure, and exposure time can be based on the various process parameters described above, the details of which are not repeated herein for the sake of brevity.

根據實施例,暴露1120使得N前驅體流動速率與Ti前驅體流動速率之比率(N/Ti流量比)超過2。該比率可超過2、3、5、10、20、30、40、50、60、70、80、90、100,或具有在藉由此等值之任一者界定之範圍內之值。According to an embodiment, exposing 1120 is such that the ratio of N precursor flow rate to Ti precursor flow rate (N/Ti flow ratio) exceeds 2. The ratio may exceed 2, 3, 5, 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, or have a value within a range defined by any of these values.

根據實施例,暴露1120使得N前驅體流動速率超過200 sccm。例如,N前驅體流動速率可超過200 sccm、500 sccm、1000 sccm、2000 sccm、3000 sccm、4000 sccm、5000 sccm、6000 sccm、7000 sccm、8000 sccm、9000 sccm、10000 sccm,或具有在藉由此等值之任一者界定之範圍內之值。According to an embodiment, exposing 1120 is such that the N precursor flow rate exceeds 200 sccm. For example, the N precursor flow rate can exceed 200 sccm, 500 sccm, 1000 sccm, 2000 sccm, 3000 sccm, 4000 sccm, 5000 sccm, 6000 sccm, 7000 sccm, 8000 sccm, 9000 sccm, 10000 sccm, or with A value within the range defined by any of these values.

根據實施例,根據上文所描述之N/Ti流量比,暴露1120使得Ti前驅體流動速率超過100 sccm但未超過N前驅體之流動速率。例如,Ti前驅體流動速率可超過100 sccm、200 sccm、500 sccm、1000 sccm、2000 sccm、3000 sccm、4000 sccm、5000 sccm,或具有在藉由此等值之任一者界定之範圍內之值。According to an embodiment, the exposure 1120 is such that the Ti precursor flow rate exceeds 100 sccm but does not exceed the N precursor flow rate according to the N/Ti flow ratio described above. For example, the Ti precursor flow rate may exceed 100 sccm, 200 sccm, 500 sccm, 1000 sccm, 2000 sccm, 3000 sccm, 4000 sccm, 5000 sccm, or have a range defined by any of these values value.

圖12A繪示根據實施例之具有相對較高(111)結晶紋理之所得TiN薄膜之實驗X射線繞射光譜。X射線繞射光譜取自下文表1中所展示之實例1至實例4。圖12B係繪示自圖12A之X射線繞射光譜獲得之對應於TiN之(111)晶向之X射線繞射峰之峰值高度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度之實驗比率的圖表。所繪示之TiN薄膜僅作為實例展示,且實施例並不限於此。根據實施例,N前驅體流動速率範圍及Ti前驅體流動速率範圍使得TiN薄膜相對於可比較薄膜(例如,具有類似厚度之TiN)具有相對較高(111)結晶紋理,該可比較薄膜藉由使半導體基板暴露至各包括至上文所描述之Ti前驅體流動速率範圍之外的不同Ti前驅體流動速率範圍之暴露及至上文所描述之N前驅體流動速率範圍之外的不同N前驅體流動速率範圍之暴露之週期性氣相沈積循環而形成。增加之(111)紋理之程度可使用(例如) X射線繞射來量測。例如,不同X射線峰值之相對強度可提供紋理化程度之至少半定量指示。根據實施例形成之TiN薄膜有利地具有相對較高(111)結晶紋理,使得薄膜之X射線光譜具有對應於(111)晶向之X射線繞射峰之峰值高度或強度與對應於(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。例如,此比率可超過0.4、0.6、0.8、1.0、1.2、1.4、1.6、1.8、2.0,或在藉由此等值之任一者界定之範圍內之值。在表1中概述選定實驗前驅體流動條件及對應比率量測值。Figure 12A shows the experimental X-ray diffraction spectrum of the resulting TiN thin film with relatively high (111) crystalline texture according to an embodiment. X-ray diffraction spectra were taken from Examples 1 to 4 shown in Table 1 below. FIG. 12B shows the peak height of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the peak value of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN obtained from the X-ray diffraction spectrum of FIG. 12A Graph of the experimental ratio of height. The depicted TiN thin film is shown as an example only, and the embodiments are not limited thereto. According to an embodiment, the N precursor flow rate range and the Ti precursor flow rate range enable TiN films to have a relatively high (111) crystalline texture relative to a comparable film (e.g., TiN of similar thickness) obtained by Exposing the semiconductor substrate to exposures each including to a different Ti precursor flow rate range outside the Ti precursor flow rate range described above and to a different N precursor flow outside the N precursor flow rate range described above Formed by periodic vapor deposition cycles of exposure over a range of rates. The degree of increased (111) texture can be measured using, for example, X-ray diffraction. For example, the relative intensities of different X-ray peaks can provide at least a semi-quantitative indication of the degree of texturing. The TiN thin film formed according to the embodiment advantageously has a relatively high (111) crystal texture, so that the X-ray spectrum of the thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation and the peak height or intensity corresponding to the (200) crystal orientation. The ratio of the peak height or intensity of the X-ray diffraction peak exceeding 0.4. For example, this ratio may exceed 0.4, 0.6, 0.8, 1.0, 1.2, 1.4, 1.6, 1.8, 2.0, or a value within the range defined by any of these values. Selected experimental precursor flow conditions and corresponding ratio measurements are summarized in Table 1.

圖13係根據實施例之具有相對較高(111)結晶紋理之TiN薄膜之實驗厚度及電阻率量測值的圖表。對於在表1中列出之實例1至實例4,針對相同數目個循環,增加N/Ti流量比減少厚度。出乎意料的是,不同於習知方法,增加N/Ti流量比(此繼而減小厚度)降低TiN薄膜之電阻率。在本發明之前,減小厚度與增加電阻率相關聯,增加電阻率與在由TiCl 4形成之相對較薄TiN薄膜中之氯之相對較高量相關。所繪示之TiN薄膜僅作為實例展示,且實施例不限於此。有利的是,根據實施例形成之TiN膜之電阻率小於約200 μΩ-cm或上文所描述之任何值。在表1中概述選定實驗前驅體流動條件以及厚度及電阻率之對應量測值。 表1 實例    TiCl 4流動速率    (sccm) NH 3流動速率    (sccm) NH 3/TiCl 4流動速率比 厚度       (Å) 電阻率       (μΩcm) 薄片電阻    (Ω/sq)    (111) X射線峰值 / (200) X射線峰值比 1 140 500 3.6 268 159 59.3 0.43 2 140 1000 7.1 265 145 54.5 0.56 3 140 2000 14.3 261 136 52.2 0.75 4 140 4000 28.6 261 129 49.4 1.39 13 is a graph of experimental thickness and resistivity measurements of TiN films with relatively high (111) crystalline texture, according to an embodiment. For Examples 1 to 4 listed in Table 1, increasing the N/Ti flow ratio decreased thickness for the same number of cycles. Unexpectedly, unlike conventional methods, increasing the N/Ti flow ratio (which in turn reduces the thickness) reduces the resistivity of TiN thin films. Prior to the present invention, decreasing thickness was associated with increasing resistivity associated with relatively higher amounts of chlorine in relatively thin TiN films formed from TiCl4 . The depicted TiN thin film is shown as an example only, and the embodiments are not limited thereto. Advantageously, TiN films formed according to embodiments have a resistivity of less than about 200 μΩ-cm, or any of the values described above. The selected experimental precursor flow conditions and corresponding measurements of thickness and resistivity are summarized in Table 1 . Table 1 example TiCl 4 flow rate (sccm) NH 3 flow rate (sccm) NH 3 /TiCl 4 flow rate ratio Thickness (Å) Resistivity (μΩcm) Sheet Resistance (Ω/sq) (111) X-ray peak/(200) X-ray peak ratio 1 140 500 3.6 268 159 59.3 0.43 2 140 1000 7.1 265 145 54.5 0.56 3 140 2000 14.3 261 136 52.2 0.75 4 140 4000 28.6 261 129 49.4 1.39

圖14係根據實施例之具有實質上相同厚度及優先(111)結晶紋理之TiN薄膜之實驗硬度及模量量測值的圖表。圖15係根據實施例之針對兩種不同厚度具有相對較高(111)結晶紋理之TiN薄膜之實驗硬度量測值的圖表。根據實施例,增加N/Ti流量比(此繼而減小厚度)增加TiN薄膜之楊氏模量及硬度。所繪示之TiN薄膜僅作為實例展示,且實施例不限於此。有利的是,根據實施例形成之TiN膜之硬度超過6 GPa。例如,硬度可超過6 GPa、10 GPa、14 GPa、18 GPa、22 GPa、25 GPa,或具有在藉由此等值之任一者界定之範圍內之值。有利的是,根據實施例形成之TiN膜之彈性或楊氏模量超過150 GPa。例如,楊氏模量可超過150 GPa、170 GPa、190 GPa、210 GPa、230 GPa、250 GPa、270 GPa、300 GPa,或具有在藉由此等值之任一者界定之範圍內之值。14 is a graph of experimental hardness and modulus measurements of TiN thin films having substantially the same thickness and a preferential (111) crystalline texture, according to an embodiment. 15 is a graph of experimental hardness measurements for two different thicknesses of TiN thin films with relatively high (111) crystalline texture, according to an embodiment. According to an embodiment, increasing the N/Ti flow ratio (which in turn reduces the thickness) increases the Young's modulus and hardness of the TiN film. The depicted TiN thin film is shown as an example only, and the embodiments are not limited thereto. Advantageously, the hardness of the TiN film formed according to the embodiments exceeds 6 GPa. For example, hardness may exceed 6 GPa, 10 GPa, 14 GPa, 18 GPa, 22 GPa, 25 GPa, or have a value within a range defined by any of these values. Advantageously, the elasticity or Young's modulus of TiN films formed according to the embodiments exceeds 150 GPa. For example, the Young's modulus may exceed 150 GPa, 170 GPa, 190 GPa, 210 GPa, 230 GPa, 250 GPa, 270 GPa, 300 GPa, or have a value within the range defined by any of these values .

根據本文中所描述之方法,降低沈積壓力增加對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度之比率。此係在圖16中進行繪示,圖16繪示根據實施例之在不同暴露壓力下形成且具有優先(111)結晶紋理之TiN薄膜之實驗X射線光譜。所繪示之TiN薄膜僅作為實例展示,且實施例不限於此。特定言之,X射線繞射輪廓係針對具有相同厚度但在兩種不同暴露壓力(即,5托及3托)下形成之TiN膜獲取。結果表明,較低壓力可導致(111)結晶紋理之進一步增加。然而,本發明者已認知,在一些境況下,較低暴露壓力可導致損害之階梯覆蓋率。因此,在此等境況中,根據實施例,在形成1130 (圖11)具有相對較高(111)結晶紋理之TiN薄膜之後,方法1100 (圖11)可進一步包含藉由使半導體基板暴露至各包括至第二Ti前驅體之暴露及至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在TiN薄膜上形成第二TiN薄膜,其中相對於在一或多個第一週期性氣相沈積循環期間至Ti前驅體及N前驅體之一或兩者之對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之暴露係在較高壓力下。對應於形成1130 (圖11) TiN薄膜及形成第二TiN薄膜之其他暴露條件可根據上文關於圖3A、圖3B及圖4所描述之暴露條件之任一者。According to the methods described herein, reducing the deposition pressure increases the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN. Strength ratio. This is illustrated in FIG. 16 , which shows experimental X-ray spectra of TiN thin films formed under different exposure pressures and having a preferential (111 ) crystalline texture, according to an embodiment. The depicted TiN thin film is shown as an example only, and the embodiments are not limited thereto. Specifically, X-ray diffraction profiles were taken for TiN films with the same thickness but formed at two different exposure pressures (ie, 5 Torr and 3 Torr). The results show that lower pressure can lead to further increase of (111) crystalline texture. However, the inventors have recognized that, in some circumstances, lower exposure pressures can result in stepped coverage of damage. Therefore, in such circumstances, according to an embodiment, after forming 1130 ( FIG. 11 ) a TiN thin film having a relatively high (111) crystalline texture, the method 1100 ( FIG. 11 ) may further comprise exposing the semiconductor substrate to various one or more second periodic vapor deposition cycles comprising exposure to a second Ti precursor and exposure to a second N precursor to form a second TiN thin film on the TiN thin film, wherein relative to the one or more first Corresponding exposure to one or both of the Ti precursor and the N precursor during one periodic vapor deposition cycle, to the second Ti precursor and the first Ti precursor during the one or more second periodic vapor deposition cycles Exposure to one or both of the two N precursors is at higher pressure. Other exposure conditions corresponding to forming 1130 ( FIG. 11 ) the TiN film and forming the second TiN film may be according to any of the exposure conditions described above with respect to FIGS. 3A , 3B and 4 .

圖17繪示根據實施例之具有增加之(111)結晶紋理之TiN薄膜之氯濃度深度輪廓。深度輪廓係使用二次離子質譜法獲得。經量測之薄膜對應於表1中列出之實例1至實例4。如上文所描述,針對相同數目個循環,增加N/Ti流量比減小厚度。出乎意料的是,不同於習知方法,增加N/Ti流量比(此繼而減小厚度)降低TiN薄膜之電阻率。圖17繪示電阻率隨厚度減小而降低之此出乎意料趨勢與氯濃度降低相關。對於實例1至實例4所涵蓋之N/Ti流量比之範圍,氯之量可減少50%以上。例如,在約10 nm處,對於實例1至實例4,氯濃度分別量測為7.2x10 20/cm 3、6.1x10 20/cm 3、5.1x10 20/cm 3及3.5x10 20/cm 3。在本發明之前,厚度減小與氯含量增加相關聯,氯含量增加與相對較高電阻率相關。 具有增加之 (111) 結晶紋理之雙層 TiN 薄膜之原子層沈積 17 shows the chlorine concentration depth profile of a TiN thin film with increased (111) crystalline texture according to an embodiment. Depth profiles were obtained using secondary ion mass spectrometry. The measured films correspond to Examples 1 to 4 listed in Table 1. As described above, increasing the N/Ti flow ratio reduces thickness for the same number of cycles. Unexpectedly, unlike conventional methods, increasing the N/Ti flow ratio (which in turn reduces the thickness) reduces the resistivity of TiN thin films. Figure 17 shows that the unexpected trend of decreasing resistivity with decreasing thickness correlates with decreasing chlorine concentration. For the range of N/Ti flow ratios covered by Examples 1 to 4, the amount of chlorine can be reduced by more than 50%. For example, at about 10 nm, chlorine concentrations were measured as 7.2x10 20 /cm 3 , 6.1x10 20 /cm 3 , 5.1x10 20 /cm 3 , and 3.5x10 20 /cm 3 for Examples 1 to 4, respectively. Prior to the present invention, reduced thickness was associated with increased chlorine content, which was associated with relatively higher resistivity. Atomic Layer Deposition of Bilayer TiN Thin Films with Increased (111) Crystalline Texture

如上文所描述,高N/Ti流量比及/或低壓力可增加所得TiN薄膜之(111)紋理。然而,以與上文關於低壓沈積之TiN薄膜所描述類似之方式,高N/Ti流量比可導致相對較低階梯覆蓋率。為補償,可需要具有雙層程序,其中在具有高(111)紋理之第一TiN薄膜上生長第二TiN薄膜。As described above, a high N/Ti flow ratio and/or low pressure can increase the (111) texture of the resulting TiN film. However, high N/Ti flow ratios can result in relatively low step coverage in a manner similar to that described above for low pressure deposited TiN films. To compensate, it may be desirable to have a bilayer procedure where a second TiN film is grown on a first TiN film with a high (111) texture.

根據此等實施例,方法包括藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜。此外,方法包括藉由使半導體基板暴露至各包括以第二Ti前驅體流動速率至第二Ti前驅體之暴露及以第二N前驅體流動速率至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在該TiN薄膜上形成第二TiN薄膜。方法使得該TiN薄膜及該第二TiN薄膜之一或兩者具有優先(111)結晶紋理,使得TiN薄膜及第二TiN薄膜之一或兩者之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。According to these embodiments, the method includes exposing the semiconductor substrate to one or more periodic gases each comprising exposure to the Ti precursor at a Ti precursor flow rate and exposure to the N precursor at a N precursor flow rate. phase deposition cycle to form a TiN thin film on the semiconductor substrate. Additionally, the method includes exposing the semiconductor substrate to one or more of exposure to the second Ti precursor at a second Ti precursor flow rate and exposure to the second N precursor at a second N precursor flow rate, each comprising: A second periodic vapor deposition cycle is used to form a second TiN thin film on the TiN thin film. The method makes one or both of the TiN thin film and the second TiN thin film have a preferential (111) crystal texture, so that the X-ray spectrum of one or both of the TiN thin film and the second TiN thin film has a (111) crystal texture corresponding to TiN. The ratio of the peak height or intensity of the X-ray diffraction peak of the orientation to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN exceeds 0.4.

根據一些其他實施例,一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法包括藉由使半導體基板暴露至各包括以第一Ti前驅體流動速率至第一Ti前驅體之暴露及以第一N前驅體流動速率至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環而在第一壓力下在該半導體基板上形成第一TiN薄膜。該第一TiN薄膜具有結晶紋理,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。此外,該方法包括藉由使該半導體基板暴露至各包括以第二Ti前驅體流動速率至第二Ti前驅體之暴露及以第二N前驅體流動速率至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在高於該第一壓力之第二壓力下在該第一TiN薄膜上形成第二TiN薄膜。According to some other embodiments, a method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process includes exposing a semiconductor substrate to a first Ti precursor at a first Ti precursor flow rate. A first TiN thin film is formed on the semiconductor substrate at a first pressure by one or more first periodic vapor deposition cycles of exposure to a precursor and exposure to the first N precursor at a first N precursor flow rate. The first TiN thin film has a crystalline texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the X-ray corresponding to the (200) crystal orientation of TiN The ratio of the peak height or intensity of diffraction peaks exceeding 0.4. Additionally, the method includes exposing the semiconductor substrate to one of exposure to a second Ti precursor at a second Ti precursor flow rate and exposure to a second N precursor at a second N precursor flow rate by exposing the semiconductor substrate to or a plurality of second periodic vapor deposition cycles to form a second TiN film on the first TiN film at a second pressure higher than the first pressure.

有利的是,生長於TiN薄膜上之第二TiN薄膜可受益於底層第一TiN薄膜之高(111)紋理。在此等境況下,第二TiN薄膜亦可具有相對較高(111)紋理,儘管事實上,若生長於不具有底層第一TiN薄膜之(111) TiN紋理之另一表面上,則第二TiN薄膜可不具有相對較高(111)紋理。例如,若生長於不同表面(例如,除TiN以外之材料或不具有相對較高(111)紋理之TiN) (諸如絕緣膜,諸如SiO 2、Si或其他材料)上,則第二TiN薄膜可不具有相對較高(111)紋理。例如,若生長於另一表面上,則第二TiN層可具有結晶紋理,使得TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度實質上小於0.4 (例如,0.3、0.2、0.1或在藉由此等值之任一者界定之範圍內之值)的比率。此係因為底層TiN薄膜之經紋理化表面可用作第二TiN薄膜之模板,使得第二TiN薄膜可在增加階梯覆蓋率之條件下(例如,在如上文關於各種兩步沈積程序所描述之高壓下)生長。 Advantageously, the second TiN film grown on the TiN film can benefit from the high (111) texture of the underlying first TiN film. Under these circumstances, the second TiN film may also have a relatively high (111) texture, despite the fact that if grown on another surface that does not have the (111) TiN texture of the underlying first TiN film, the second TiN films may not have a relatively high (111) texture. For example, if grown on a different surface (e.g., a material other than TiN or TiN that does not have a relatively high (111) texture), such as an insulating film such as SiO 2 , Si, or other materials, the second TiN film may not Has a relatively high (111) texture. For example, if grown on another surface, the second TiN layer can have a crystalline texture such that the X-ray spectrum of the TiN thin film has a peak height or intensity corresponding to the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and corresponding to The ratio of peak heights or intensities of the X-ray diffraction peaks of the (200) crystal orientation of TiN to substantially less than 0.4 (eg, 0.3, 0.2, 0.1, or a value within a range defined by any of these values). This is because the textured surface of the underlying TiN film can be used as a template for the second TiN film so that the second TiN film can be formed under conditions of increased step coverage (e.g., as described above for the various two-step deposition procedures). under high pressure) to grow.

例如,第二TiN薄膜可在如上文所描述之高壓(例如,大於3托或5托)下(例如)根據關於圖3A及圖3B所描述之各種兩步程序形成。例如,藉由紋理化第一TiN薄膜以具有相對較高(111)定向,初始膜生長可實質上以(111)紋理有利模式繼續進行,此有利地導致如上文所描述之改良之機械性質及電阻率。另一方面,藉由隨後在薄膜之第二部分之沈積期間使基板在相對較高壓力(例如,大於3托)下暴露至Ti及/或N前驅體,薄膜之後一部分或第二TiN薄膜可有利地以相對於具有相對較高(111)紋理之第一TiN薄膜或相對於藉由在相對較低壓力(例如,小於3托或小於1托)下使基板暴露至Ti及/或N前驅體而沈積之TiN薄膜較高之保形度或階梯覆蓋率生長。For example, the second TiN film can be formed at high pressures as described above (eg, greater than 3 Torr or 5 Torr), eg, according to the various two-step procedures described with respect to FIGS. 3A and 3B . For example, by texturing the first TiN film to have a relatively high (111) orientation, initial film growth can proceed substantially in a (111) texture-favorable mode, which advantageously results in the improved mechanical properties and resistivity. On the other hand, by subsequently exposing the substrate to Ti and/or N precursors at a relatively high pressure (e.g., greater than 3 Torr) during deposition of the second portion of the film, a later portion of the film or a second TiN film can be Advantageously, with respect to a first TiN thin film having a relatively high (111) texture or with respect to a TiN precursor by exposing the substrate to a Ti and/or N precursor at a relatively low pressure (e.g., less than 3 Torr or less than 1 Torr) TiN films deposited in bulk can grow with higher conformality or step coverage.

另外,由於TiN薄膜之第一部分具有相對較高(111)紋理,故薄膜之第二部分可使用第一部分作為模板繼續以逐層方式生長。第二TiN薄膜可具有相對於底層第一TiN薄膜較低或可比較的(111)紋理。In addition, since the first portion of the TiN film has a relatively high (111) texture, the second portion of the film can continue to grow in a layer-by-layer manner using the first portion as a template. The second TiN film may have a lower or comparable (111) texture relative to the underlying first TiN film.

作為最終結果,當沈積於特定表面(例如,包括非金屬表面之表面)上時,包括藉由根據本文中所揭示之方法沈積相對較高(111)紋理化之第一TiN薄膜接著第二TiN薄膜而沈積之第一及第二部分之薄膜有利地具有優於使用單一步驟形成於相同表面上之薄膜層之表面粗糙度及保形性之組合。替代性地或此外,部分歸因於改良之平滑度及保形性,薄膜具有相較於藉由一些現有方法形成之TiN層相對較低之電阻率。 應用 As a final result, when deposited on a particular surface (e.g., a surface including a non-metallic surface), it involves depositing a relatively highly (111) textured first TiN film followed by a second TiN film according to the methods disclosed herein. The thin films of the first and second portions deposited as thin films advantageously have a combination of surface roughness and conformality superior to thin film layers formed on the same surface using a single step. Alternatively or additionally, due in part to the improved smoothness and conformality, the thin films have relatively lower resistivity compared to TiN layers formed by some prior methods. application

根據本文中所揭示之各項實施例使用不同暴露壓力形成之包括TiN之薄膜可用於各種應用中,尤其在基板包括可受益於如本文中所揭示之TiN層之各種有利特性之相對較高縱橫比結構及/或非金屬表面之情況下。實例性應用包含在具有超過1、2、5、10、20、50、100、200或在藉由此等值之任一者界定之範圍內之值之縱橫比(例如,定義為深度除以頂部寬度之比率)之通孔、孔、溝渠、腔或類似結構中之沈積。Thin films comprising TiN formed using different exposure pressures according to various embodiments disclosed herein can be used in a variety of applications, especially where substrates include relatively high aspect ratios that can benefit from the various advantageous properties of the TiN layer as disclosed herein. than in the case of structures and/or non-metallic surfaces. Exemplary applications include aspect ratios (e.g., defined as depth divided by Deposition in vias, holes, trenches, cavities, or similar structures.

藉由實例,圖10示意性地繪示在用於接觸結構(例如,源極或汲極接觸件)之形成於可經重度摻雜之主動半導體基板區域上之擴散阻障之背景內容中之應用。繪示半導體裝置1000之部分,其包含基板1004,包括介電材料(諸如氧化物或氮化物)之介電質層1008 (例如,層間或金屬間介電質(ILD)層)形成於基板1004上。為形成至基板1004之各種區域(包含各種經摻雜區域,例如,源極及汲極區域)之接觸件,可形成穿過介電質層1008之通孔或溝渠。該通孔或該溝渠可暴露各種非金屬表面,例如,通孔之包括基板表面(例如,矽基板表面)之經暴露底表面,以及介電質側壁。可用根據本文中所描述之各項實施例形成之TiN層之第一部分(對應於圖3B中之第一部分370)接著用第二部分(對應於圖3B中之第二部分380)保形地塗佈通孔之底表面及側表面。根據本文中所揭示之各項實施例,首先可在通孔之內表面上直接形成保形第一部分,接著形成保形第二TiN層。此後,可用金屬(例如,W、Al或Cu)填充經加襯裡通孔以形成接觸插塞1016。例如,可藉由CVD使用(例如) WF 6用鎢填充通孔。 By way of example, FIG. 10 schematically illustrates in the context of a diffusion barrier for a contact structure (eg source or drain contact) formed on an active semiconductor substrate region that may be heavily doped. application. Depicted is a portion of a semiconductor device 1000 comprising a substrate 1004 on which a dielectric layer 1008 (eg, an interlayer or intermetal dielectric (ILD) layer) comprising a dielectric material such as an oxide or nitride is formed superior. To form contacts to various regions of the substrate 1004 , including various doped regions such as source and drain regions, vias or trenches may be formed through the dielectric layer 1008 . The via or the trench can expose various non-metallic surfaces, for example, the exposed bottom surface of the via including the substrate surface (eg, a silicon substrate surface), and dielectric sidewalls. A first portion (corresponding to first portion 370 in FIG. 3B ) of a TiN layer formed according to embodiments described herein may then be conformally coated with a second portion (corresponding to second portion 380 in FIG. 3B ). Bottom surface and side surface of through hole. According to various embodiments disclosed herein, the conformal first portion may first be formed directly on the inner surface of the via, followed by the formation of the conformal second TiN layer. Thereafter, the lined via hole may be filled with a metal (eg, W, Al, or Cu) to form a contact plug 1016 . For example, vias can be filled with tungsten by CVD using, for example, WF 6 .

出於各種原因,根據實施例形成之阻障層1012可為有利的。特定言之,歸因於藉由ALD形成之阻障層1012之保形性質,可實質上減小在後續金屬填充程序期間之夾斷(pinching off)之傾向。另外,如上文所描述,阻障層1012可提供跨其之有效材料輸送阻礙,例如,摻雜物(B、P)自基板1004向外擴散,以及來自接觸插塞形成程序之反應物、蝕刻劑及金屬(例如,F、Cl、W或Cu)向內擴散。可藉由降低之表面粗糙度及增加之階梯覆蓋率來增強阻障效應。此外,如上文所描述,逐層生長模式可減小阻障層1012之總體接觸電阻。此外,歸因於降低之膜粗糙度,可形成相對較薄阻障層1012,同時仍完成其所要阻障功能,從而導致接觸電阻進一步降低。Barrier layer 1012 formed according to embodiments may be advantageous for a variety of reasons. In particular, due to the conformal nature of the barrier layer 1012 formed by ALD, the propensity for pinching off during subsequent metal fill processes can be substantially reduced. In addition, as described above, the barrier layer 1012 can provide an effective barrier to material transport across it, for example, outdiffusion of dopants (B, P) from the substrate 1004, and reactants from the contact plug formation process, etch Agents and metals (eg, F, Cl, W or Cu) diffuse inwardly. The barrier effect can be enhanced by reduced surface roughness and increased step coverage. Furthermore, as described above, the layer-by-layer growth mode can reduce the overall contact resistance of the barrier layer 1012 . Furthermore, due to the reduced film roughness, a relatively thinner barrier layer 1012 can be formed while still fulfilling its intended barrier function, resulting in a further reduction in contact resistance.

根據本文中所揭示之各項實施例形成之TiN層之其他應用包含(僅舉幾例)形成於凹入基板中之導電結構(例如,埋藏式電極或線)、電極(例如,DRAM電容器電極或閘極電極)、用於較高金屬層級之金屬化阻障(例如,用於Cu接觸件/線之通孔/溝渠中之阻障)、高縱橫比垂直棒狀電極或用於三維記憶體之通孔及矽穿孔(TSV)。 實例性實施例 I 1. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜, 其中該N前驅體流動速率與該Ti前驅體流動速率之比率超過3。 2. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以第一N前驅體流動速率至第一N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜, 其中該N前驅體流動速率超過200 sccm。 3. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以Ti前驅體流動速率範圍內之Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率範圍內之N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜, 其中該N前驅體流動速率範圍及該Ti前驅體流動速率範圍使得該TiN薄膜相對於藉由使該半導體基板暴露至各包括至該Ti前驅體流動速率範圍之外之不同Ti前驅體流動速率範圍內之該Ti前驅體之暴露及至該N前驅體流動速率範圍之外之不同N前驅體流動速率範圍內之該N前驅體之暴露之週期性氣相沈積循環而形成之另一TiN薄膜具有優先(111)結晶紋理。 4. 如以上實施例中任一項之方法,其中該N前驅體流動速率與該Ti前驅體流動速率之該比率係2至100。 5. 如以上實施例中任一項之方法,其中該N前驅體流動速率係200 sccm至10,000 sccm。 6. 如以上實施例中任一項之方法,其中該Ti前驅體流動速率係100 sccm至5000 sccm。 7. 如以上實施例中任一項之方法,其中該TiN薄膜具有優先(111)結晶紋理,使得該TiN薄膜之X射線光譜具有對應於(111)晶向之X射線繞射峰之峰值高度或強度與對應於(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 8. 如以上實施例中任一項之方法,其中該TiN薄膜具有超過6 GPa之硬度。 9. 如以上實施例中任一項之方法,其中該TiN薄膜具有超過150 GPa之楊氏模量。 10. 如以上實施例中任一項之方法,其進一步包括: 藉由使該半導體基板暴露至各包括至第二Ti前驅體之暴露及至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在該TiN薄膜上形成第二TiN薄膜, 其中相對於在該一或多個週期性氣相沈積循環期間至該Ti前驅體及該N前驅體之一或兩者之對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之暴露係在較高壓力下。 11. 如實施例10之方法,其中在該一或多個週期性氣相沈積循環期間至該Ti前驅體及該N前驅體之一或兩者之該等暴露係在小於約5托之反應器壓力下,且其中在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之該等暴露係在大於約5托之反應器壓力下。 12. 如實施例10或11之方法,其中相對於在該一或多個週期性氣相沈積循環期間至該Ti前驅體及該N前驅體之各者之該對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之各者之該暴露係在較高壓力下。 13. 如實施例10至12中任一項之方法,其中形成該TiN薄膜包括以包括該半導體基板至該Ti前驅體之暴露及至該N前驅體之暴露之該等週期性氣相沈積循環之每一者小於0.3 Å之第一沈積速率進行沈積,且其中形成該第二TiN薄膜包括以包括該半導體基板至該第二Ti前驅體之暴露及至該第二N前驅體之暴露之該等第二週期性氣相沈積循環之每一者大於0.3 Å之第二沈積速率進行沈積。 14. 如以上實施例中任一項之方法,其中該薄膜之均方根表面粗糙度小於該薄膜之厚度之約8%。 15. 如實施例10至14中任一項之方法,其中形成該TiN薄膜及該第二TiN薄膜包括藉由熱週期性氣相沈積進行沈積。 16. 如實施例10至15中任一項之方法,其中形成該TiN薄膜包括使半導體表面及絕緣體表面之一或兩者直接暴露至該一或多個週期性氣相沈積循環。 17. 如實施例10至16中任一項之方法,其中形成該TiN薄膜及該第二TiN薄膜之一或兩者包括以逐層生長模式生長。 18. 如實施例10至17中任一項之方法,其中形成該TiN薄膜包括使該半導體基板交替地暴露至1個至50個週期性氣相沈積循環。 19. 如實施例10至18中任一項之方法,其中形成該TiN薄膜及該第二TiN薄膜包括在400 oC與600 oC之間的溫度下形成。 20. 如以上實施例中任一項之方法,其中該半導體基板包括含有內表面之溝渠或通孔,該內表面包括在具有超過1之縱橫比之溝渠或通孔中之非金屬側壁表面,且其中形成該薄膜包括保形地加襯裡於該內表面,其中形成於該溝渠或該通孔之高度之下25%及該溝渠或該通孔之該高度之上25%上之該薄膜之厚度之比率超過0.9。 21. 如以上實施例中任一項之方法,其中該薄膜之電阻率小於約200 μΩ-cm。 22. 如實施例10至21中任一項之方法,其中該Ti前驅體係與該第二Ti前驅體相同且該N前驅體係與該第二N前驅體相同。 23. 如實施例1至9中任一項之方法,該方法包括: 提供包括具有超過1之縱橫比之溝渠或通孔之該半導體基板; 藉由使該半導體基板暴露至該一或多個週期性氣相沈積以在該溝渠或該通孔中形成該TiN薄膜而在該溝渠或該通孔中形成該薄膜;及 進一步使該半導體基板暴露至各包括至第二Ti前驅體之暴露及至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環以在該TiN薄膜上形成第二TiN薄膜,其中相對於在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之對應暴露,在該一或多個週期性氣相沈積循環期間至該Ti前驅體及該N前驅體之一或兩者之暴露係在不同壓力下。 24. 如實施例23之方法,其中相對於在該一或多個週期性氣相沈積循環期間至該Ti前驅體及該N前驅體之一或兩者之對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之暴露係在較高壓力下。 25. 如實施例23或24之方法,其中相對於在該一或多個週期性氣相沈積循環期間至該Ti前驅體及該N前驅體之一或兩者之對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之暴露係在5倍或更大之壓力下。 26. 如實施例23至25中任一項之方法,其中形成該TiN薄膜包括使該半導體基板交替地暴露至1個至50個週期性氣相沈積循環。 27. 如實施例23至26中任一項之方法,其中形成該TiN薄膜包括使該半導體基板暴露至第一數目個該一或多個週期性氣相沈積循環,且其中形成第二部分包括使該半導體基板暴露至大於該一或多個週期性氣相沈積循環之該第一數目的兩倍的第二數目個第二週期性氣相沈積循環。 28. 如實施例23至27中任一項之方法,其中該薄膜之均方根表面粗糙度小於該薄膜之厚度之約8%。 29. 如實施例23至28中任一項之方法,其中形成該TiN層包括藉由熱週期性氣相沈積在400 oC與600 oC之間的溫度下形成。 30. 如實施例23至29中任一項之方法,其中該溝渠或該通孔具有超過5之縱橫比及包括非金屬側壁表面之內表面,且其中形成該薄膜包括保形地加襯裡於該內表面,其中形成於該溝渠或該通孔之高度之下25%及該溝渠或該通孔之該高度之上25%上之該薄膜之厚度之比率超過0.9。 31. 如實施例23至29中任一項之方法,其中該Ti前驅體係與該第二Ti前驅體相同且該N前驅體係與該第二N前驅體相同。 32. 一種半導體結構,其包括: 半導體基板,其包括在具有超過5之縱橫比之溝渠或通孔中之非金屬側壁表面;及 包括TiN之薄膜,其保形地加襯裡於該非金屬側壁表面, 其中該薄膜具有優先(111)結晶紋理,使得該薄膜之X射線光譜具有對應於(111)晶向之X射線繞射峰之峰值高度或強度與對應於(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 33. 如實施例32之半導體結構,其中該比率超過1.3。 34. 如實施例32及33之半導體結構,其中該薄膜具有超過6 GPa之硬度。 35. 如實施例32至34中任一項之半導體結構,其中該薄膜具有超過150 GPa之楊氏模量。 36. 如實施例32至35中任一項之半導體結構,其中形成於該溝渠或該通孔之高度之下25%及該溝渠或該通孔之該高度之上25%上之該薄膜之厚度之比率超過0.9。 37. 如實施例32至36中任一項之半導體結構,其中該溝渠或該通孔具有超過10之縱橫比。 38. 如實施例32至37中任一項之半導體結構,其中形成於該非金屬表面上之該薄膜之均方根表面粗糙度小於基於該薄膜之平均厚度之約8%。 39. 如實施例32至38中任一項之半導體結構,其中該溝渠或該通孔具有介電質側壁。 40. 如實施例32至39中任一項之半導體結構,其中該溝渠或該通孔具有暴露該半導體基板之半導體材料之底表面。 41. 如實施例32至40中任一項之半導體結構,其中該薄膜具有小於約200 μΩ-cm之電阻率。 42. 如實施例32至41中任一項之半導體結構,其中用該薄膜加襯裡之該溝渠或該通孔係用包括鎢之金屬填充。 實例性實施例 II 1. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜, 其中該N前驅體流動速率與該Ti前驅體流動速率之比率(N/Ti流量比)超過3,且 其中該方法形成具有結晶紋理之該TiN薄膜,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 2. 如實施例1之方法,其中該N/Ti流量比係3至100。 3. 如實施例1或2之方法,其中該方法使得增加該N/Ti流量比減小該TiN薄膜之厚度。 4. 如實施例1至3中任一項之方法,其中增加該N/Ti流量比降低該TiN薄膜之電阻率。 5. 如實施例1至4中任一項之方法,其中該方法使得增加該N/Ti流量比增加該TiN薄膜之楊氏模量。 6. 如實施例5之方法,其中增加該楊氏模量包括增加至超過150 GPa之值。 7. 如實施例1至6中任一項之方法,其中該方法使得增加該N/Ti流量比增加該TiN薄膜之硬度。 8. 如實施例7之方法,其中增加該硬度包括增加至超過6 GPa之值。 9. 如實施例1至8中任一項之方法,其中增加該N/Ti流量比降低該TiN薄膜之氯含量。 10. 如實施例1至9中任一項之方法,其中該方法使得降低沈積壓力增加對應於TiN之該(111)晶向之該X射線繞射峰之該峰值高度或該強度與對應於TiN之該(200)晶向之該X射線繞射峰之該峰值高度或該強度之該比率。 11. 如實施例1至10中任一項之方法,其中該N前驅體流動速率係500 sccm至10,000 sccm。 12. 如實施例1至11中任一項之方法,其中該Ti前驅體流動速率係100 sccm至5000 sccm。 13. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以Ti前驅體流動速率至Ti前驅體之暴露及以N前驅體流動速率至N前驅體之暴露之一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜, 其中該N前驅體流動速率超過500 sccm,且 其中該方法形成具有結晶紋理之該TiN薄膜,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 14. 如實施例13之方法,該N前驅體流動速率與該Ti前驅體流動速率之比率(N/Ti流量比)係3至100。 15. 如實施例14之方法,其中該方法使得增加該N/Ti流量比減小該TiN薄膜之厚度。 16. 如實施例15之方法,其中減小該厚度降低該TiN薄膜之電阻率。 17. 如實施例15至16中任一項之方法,其中減小該厚度增加該TiN薄膜之楊氏模量。 18. 如實施例17之方法,其中增加該楊氏模量包括增加至超過150 GPa之值。 19. 如實施例15至18中任一項之方法,其中減小該厚度增加該TiN薄膜之硬度。 20. 如實施例19之方法,其中增加該硬度包括增加至超過6 GPa之值。 21. 如實施例15至20中任一項之方法,其中減小該厚度降低該TiN薄膜之氯含量。 22. 如實施例13至21中任一項之方法,其中降低沈積壓力增加對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度之該比率。 23. 如實施例13至22中任一項之方法,其中該N前驅體流動速率係500 sccm至10,000 sccm。 24. 如實施例13至23中任一項之方法,其中該Ti前驅體流動速率係100 sccm至5000 sccm。 25. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以第一Ti前驅體流動速率至第一Ti前驅體之暴露及以第一N前驅體流動速率至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環而在該半導體基板上形成第一TiN薄膜, 藉由使該半導體基板暴露至各包括以第二Ti前驅體流動速率至第二Ti前驅體之暴露及以第二N前驅體流動速率至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在該第一TiN薄膜上形成第二TiN薄膜, 其中該方法使得該等第一及第二TiN薄膜之一或兩者具有優先(111)結晶紋理,使得該等第一及第二TiN薄膜之該一或兩者之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 26. 如實施例25之方法,其中相對於在該一或多個第一週期性氣相沈積循環期間至該第一Ti前驅體及該第一N前驅體之一或兩者之對應暴露,在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之暴露係在較高壓力下。 27. 如實施例26之方法,該第一N前驅體流動速率與該第一Ti前驅體流動速率之第一比率(第一N/Ti流量比)及該第二N前驅體流動速率與該第二Ti前驅體流動速率之第二比率(第二N/Ti流量比)之一或兩者係3至100。 28. 如實施例27之方法,其中該方法使得增加該第一N/Ti流量比及該第二N/Ti流量比之一或兩者減小該等第一及第二TiN薄膜之一或兩者之對應厚度。 29. 如實施例28之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之該一或兩者之對應電阻率。 30. 如實施例28或29之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應楊氏模量。 31. 如實施例30之方法,其中增加該等楊氏模量包括增加至超過150 GPa之值。 32. 如實施例28至31中任一項之方法,其中減小該等對應厚度增加該TiN薄膜及該第二TiN薄膜之對應硬度值。 33. 如實施例32之方法,其中增加該等硬度值包括增加至超過6 GPa之值。 34. 如實施例28至33中任一項之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之對應氯含量。 35. 如實施例25至34中任一項之方法,其中針對該TiN薄膜,對應於TiN之該(111)晶向之該X射線繞射峰之該峰值高度或該強度與對應於TiN之該(200)晶向之該X射線繞射峰之該峰值高度或該強度之該比率相對於針對該第二TiN薄膜之該比率較高。 36. 如實施例25至35中任一項之方法,其中在該一或多個第一週期性氣相沈積循環期間至該第一Ti前驅體及該第一N前驅體之一或兩者之該等暴露係在小於約5托之反應器壓力下,且其中在該一或多個第二週期性氣相沈積循環期間至該第二Ti前驅體及該第二N前驅體之一或兩者之該等暴露係在大於約5托之反應器壓力下。 37. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至各包括以第一Ti前驅體流動速率至第一Ti前驅體之暴露及以第一N前驅體流動速率至第一N前驅體之暴露之一或多個第一週期性氣相沈積循環而在第一壓力下在該半導體基板上形成第一TiN薄膜, 其中該第一TiN薄膜具有結晶紋理,使得該第一TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率;及 藉由使該半導體基板暴露至各包括以第二Ti前驅體流動速率至第二Ti前驅體之暴露及以第二N前驅體流動速率至第二N前驅體之暴露之一或多個第二週期性氣相沈積循環而在高於該第一壓力之第二壓力下在該第一TiN薄膜上形成第二TiN薄膜。 38. 如實施例37之方法,其中該第二壓力大於5托。 39. 如實施例37或38之方法,其中該第二TiN薄膜具有結晶紋理,使得該第二TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度之低於該第一TiN薄膜之該對應比率的比率。 40. 如實施例37至39中任一項之方法,其中該第一N前驅體流動速率與該第一Ti前驅體流動速率之至少第一比率(第一N/Ti流量比)係3至100。 41. 如實施例40之方法,其中該第二N前驅體流動速率與該第二Ti前驅體流動速率之第二比率係(第二N/Ti流量比)低於該第一N/Ti流量比。 42. 如實施例41之方法,其中該方法使得增加該第一N/Ti流量比及該第二N/Ti流量比之一或兩者減小該等第一及第二TiN薄膜之一或兩者之對應厚度。 43. 如實施例42之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之該一或兩者之對應電阻率。 44. 如實施例42之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應楊氏模量。 45. 如實施例44之方法,其中增加該等楊氏模量包括增加至超過150 GPa之值。 46. 如實施例42之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應硬度值。 47. 如實施例46之方法,其中增加該等硬度值包括增加至超過6 GPa之值。 48. 如實施例42之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之對應氯含量。 49. 如實施例37之方法,其中該第一壓力小於5托。 Other applications of TiN layers formed according to various embodiments disclosed herein include, to name a few, conductive structures (e.g., buried electrodes or lines), electrodes (e.g., DRAM capacitor electrodes) formed in recessed substrates, or gate electrodes), metallization barriers for higher metal levels (e.g. barriers in vias/trenches for Cu contacts/lines), high aspect ratio vertical rod electrodes or for 3D memory Body vias and through-silicon vias (TSVs). Exemplary Embodiment I : 1. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: One or more periodic vapor deposition cycles of exposure to Ti precursor and exposure to N precursor at a flow rate of N precursor to N precursor to form a TiN thin film on the semiconductor substrate, wherein the N precursor flow rate is the same as that of the Ti precursor The ratio of volume flow rate exceeds 3. 2. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: exposing a semiconductor substrate to a Ti precursor at a Ti precursor flow rate and A TiN film is formed on the semiconductor substrate by one or more periodic vapor deposition cycles of exposure to the first N precursor at a first N precursor flow rate, wherein the N precursor flow rate exceeds 200 sccm. 3. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: exposing a semiconductor substrate to a Ti precursor flow within a range of Ti precursor flow rates TiN film is formed on the semiconductor substrate by one or more periodic vapor deposition cycles of exposure to the Ti precursor at a flow rate of the N precursor at a flow rate of the N precursor to the N precursor, wherein The N precursor flow rate range and the Ti precursor flow rate range make the TiN thin film relative to the Ti precursor flow rate range by exposing the semiconductor substrate to different Ti precursor flow rate ranges each including to outside the Ti precursor flow rate range. Another TiN film formed by periodic vapor deposition cycles of exposure to the Ti precursor and exposure to the N precursor in a different N precursor flow rate range than the N precursor flow rate range has priority ( 111) Crystalline textures. 4. The method of any one of the above embodiments, wherein the ratio of the N precursor flow rate to the Ti precursor flow rate is 2-100. 5. The method according to any one of the above embodiments, wherein the N precursor flow rate is 200 sccm to 10,000 sccm. 6. The method according to any one of the above embodiments, wherein the Ti precursor flow rate is 100 sccm to 5000 sccm. 7. The method according to any one of the above embodiments, wherein the TiN thin film has a preferential (111) crystal texture, so that the X-ray spectrum of the TiN thin film has a peak height corresponding to an X-ray diffraction peak of the (111) crystal orientation or The ratio of the intensity to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation exceeds 0.4. 8. The method of any one of the above embodiments, wherein the TiN thin film has a hardness exceeding 6 GPa. 9. The method of any one of the preceding embodiments, wherein the TiN thin film has a Young's modulus exceeding 150 GPa. 10. The method of any one of the above embodiments, further comprising: exposing the semiconductor substrate to one or more second Ti precursors each including exposure to a second Ti precursor and exposure to a second N precursor. periodic vapor deposition cycles to form a second TiN film on the TiN film, wherein relative to one or both of the Ti precursor and the N precursor during the one or more periodic vapor deposition cycles Corresponding to exposure, exposure to one or both of the second Ti precursor and the second N precursor during the one or more second periodic vapor deposition cycles is at a higher pressure. 11. The method of embodiment 10, wherein the exposure to one or both of the Ti precursor and the N precursor during the one or more periodic vapor deposition cycles is a reaction at less than about 5 Torr under pressure, and wherein the exposure to one or both of the second Ti precursor and the second N precursor during the one or more second periodic vapor deposition cycles is greater than about 5 Torr under the reactor pressure. 12. The method of embodiment 10 or 11, wherein relative to the corresponding exposure to each of the Ti precursor and the N precursor during the one or more periodic vapor deposition cycles, during the one or more periodic vapor deposition cycles, The exposure to each of the second Ti precursor and the second N precursor during a second periodic vapor deposition cycle is at a higher pressure. 13. The method of any one of embodiments 10 to 12, wherein forming the TiN thin film comprises exposing the semiconductor substrate to the Ti precursor and exposing the N precursor to the periodic vapor deposition cycles Depositing at a first deposition rate each of less than 0.3 Å, and wherein forming the second TiN thin film includes the first deposition rates including exposure of the semiconductor substrate to the second Ti precursor and exposure to the second N precursor Depositing is performed at a second deposition rate greater than 0.3 Å for each of the two periodic vapor deposition cycles. 14. The method of any one of the preceding embodiments, wherein the root mean square surface roughness of the film is less than about 8% of the thickness of the film. 15. The method of any one of embodiments 10 to 14, wherein forming the TiN thin film and the second TiN thin film comprises depositing by thermal periodic vapor deposition. 16. The method of any one of embodiments 10 to 15, wherein forming the TiN thin film comprises directly exposing one or both of a semiconductor surface and an insulator surface to the one or more periodic vapor deposition cycles. 17. The method of any one of embodiments 10 to 16, wherein forming one or both of the TiN thin film and the second TiN thin film comprises growing in a layer-by-layer growth mode. 18. The method of any one of embodiments 10 to 17, wherein forming the TiN thin film comprises alternately exposing the semiconductor substrate to 1 to 50 periodic vapor deposition cycles. 19. The method of any one of embodiments 10 to 18, wherein forming the TiN thin film and the second TiN thin film comprises forming at a temperature between 400 ° C and 600 ° C. 20. The method of any one of the preceding embodiments, wherein the semiconductor substrate comprises a trench or via comprising an inner surface comprising non-metallic sidewall surfaces in the trench or via having an aspect ratio exceeding 1, and wherein forming the film includes conformally lining the inner surface, wherein forming the film over 25% of the height of the trench or the via and above 25% of the height of the trench or the via The thickness ratio exceeds 0.9. 21. The method of any one of the preceding embodiments, wherein the resistivity of the thin film is less than about 200 μΩ-cm. 22. The method of any one of embodiments 10 to 21, wherein the Ti precursor system is the same as the second Ti precursor and the N precursor system is the same as the second N precursor. 23. The method of any one of embodiments 1 to 9, comprising: providing the semiconductor substrate comprising trenches or vias having an aspect ratio exceeding 1; by exposing the semiconductor substrate to the one or more periodic vapor deposition to form the TiN thin film in the trench or the via; and further exposing the semiconductor substrate to each including exposure to a second Ti precursor and to Exposure of a second N precursor to one or more second periodic vapor deposition cycles to form a second TiN film on the TiN film, wherein relative to during the one or more second periodic vapor deposition cycles Corresponding exposure to one or both of the second Ti precursor and the second N precursor, to one or both of the Ti precursor and the N precursor during the one or more periodic vapor deposition cycles The exposure of the subjects was under different pressures. 24. The method of embodiment 23, wherein relative to the corresponding exposure to one or both of the Ti precursor and the N precursor during the one or more periodic vapor deposition cycles, during the one or more periodic vapor deposition cycles, Exposure to one or both of the second Ti precursor and the second N precursor during the second periodic vapor deposition cycle is at a higher pressure. 25. The method of embodiment 23 or 24, wherein relative to the corresponding exposure to one or both of the Ti precursor and the N precursor during the one or more periodic vapor deposition cycles, during the one or more periodic vapor deposition cycles, Exposure to one or both of the second Ti precursor and the second N precursor during the second plurality of periodic vapor deposition cycles is at 5 times or greater pressure. 26. The method of any one of embodiments 23 to 25, wherein forming the TiN thin film comprises alternately exposing the semiconductor substrate to 1 to 50 periodic vapor deposition cycles. 27. The method of any one of embodiments 23 to 26, wherein forming the TiN thin film comprises exposing the semiconductor substrate to a first number of the one or more periodic vapor deposition cycles, and wherein forming the second portion comprises The semiconductor substrate is exposed to a second number of second periodic vapor deposition cycles greater than twice the first number of the one or more periodic vapor deposition cycles. 28. The method of any one of embodiments 23 to 27, wherein the root mean square surface roughness of the film is less than about 8% of the thickness of the film. 29. The method of any one of embodiments 23 to 28, wherein forming the TiN layer comprises forming by thermal periodic vapor deposition at a temperature between 400 ° C and 600 ° C. 30. The method of any one of embodiments 23 to 29, wherein the trench or the via has an aspect ratio exceeding 5 and includes an inner surface that is a non-metallic sidewall surface, and wherein forming the film comprises conformally lining The inner surface, wherein the ratio of the thickness of the film formed on the lower 25% of the height of the trench or the through hole to the upper 25% of the height of the trench or the through hole exceeds 0.9. 31. The method of any one of embodiments 23 to 29, wherein the Ti precursor system is the same as the second Ti precursor and the N precursor system is the same as the second N precursor. 32. A semiconductor structure comprising: a semiconductor substrate comprising a non-metallic sidewall surface in a trench or via having an aspect ratio exceeding 5; and a thin film comprising TiN conformally lining the non-metallic sidewall surface , wherein the film has a preferential (111) crystalline texture such that the X-ray spectrum of the film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation and the X-ray diffraction peak corresponding to the (200) crystal orientation The peak height or intensity of the peaks exceeds the ratio of 0.4. 33. The semiconductor structure of embodiment 32, wherein the ratio exceeds 1.3. 34. The semiconductor structure of embodiments 32 and 33, wherein the thin film has a hardness exceeding 6 GPa. 35. The semiconductor structure of any one of embodiments 32 to 34, wherein the thin film has a Young's modulus in excess of 150 GPa. 36. The semiconductor structure of any one of embodiments 32 to 35, wherein the film is formed on the lower 25% of the height of the trench or the via and on the upper 25% of the height of the trench or the via The thickness ratio exceeds 0.9. 37. The semiconductor structure of any one of embodiments 32-36, wherein the trench or the via has an aspect ratio exceeding 10. 38. The semiconductor structure of any one of embodiments 32 to 37, wherein the root mean square surface roughness of the film formed on the non-metallic surface is less than about 8% based on the average thickness of the film. 39. The semiconductor structure of any one of embodiments 32-38, wherein the trench or the via has dielectric sidewalls. 40. The semiconductor structure of any one of embodiments 32 to 39, wherein the trench or the via has a bottom surface exposing the semiconductor material of the semiconductor substrate. 41. The semiconductor structure of any one of embodiments 32-40, wherein the thin film has a resistivity of less than about 200 μΩ-cm. 42. The semiconductor structure of any one of embodiments 32 to 41, wherein the trench or the via lined with the film is filled with a metal comprising tungsten. Exemplary Embodiment II : 1. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: One or more periodic vapor deposition cycles of exposure to Ti precursor and exposure to N precursor at a flow rate of N precursor to N precursor to form a TiN thin film on the semiconductor substrate, wherein the N precursor flow rate is the same as that of the Ti precursor The ratio of bulk flow rate (N/Ti flow ratio) exceeds 3, and wherein the method forms the TiN thin film with crystalline texture such that the X-ray spectrum of the TiN thin film has an X-ray orientation corresponding to the (111) crystal orientation of TiN The ratio of the peak height or intensity of the radiation peak to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN exceeds 0.4. 2. The method as in embodiment 1, wherein the N/Ti flow ratio is 3 to 100. 3. The method as in embodiment 1 or 2, wherein the method makes increasing the N/Ti flow ratio reduce the thickness of the TiN film. 4. The method according to any one of embodiments 1 to 3, wherein increasing the N/Ti flow ratio reduces the resistivity of the TiN thin film. 5. The method according to any one of embodiments 1 to 4, wherein the method causes increasing the N/Ti flow ratio to increase the Young's modulus of the TiN thin film. 6. The method of embodiment 5, wherein increasing the Young's modulus comprises increasing to a value exceeding 150 GPa. 7. The method according to any one of embodiments 1 to 6, wherein the method enables increasing the N/Ti flow ratio to increase the hardness of the TiN thin film. 8. The method of embodiment 7, wherein increasing the hardness comprises increasing to a value exceeding 6 GPa. 9. The method according to any one of embodiments 1 to 8, wherein increasing the N/Ti flow ratio reduces the chlorine content of the TiN film. 10. The method according to any one of embodiments 1 to 9, wherein the method reduces the deposition pressure and increases the peak height or the intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the intensity corresponding to that of TiN The peak height or the ratio of the intensity of the X-ray diffraction peak of the (200) crystal orientation. 11. The method according to any one of embodiments 1 to 10, wherein the N precursor flow rate is 500 sccm to 10,000 sccm. 12. The method according to any one of embodiments 1 to 11, wherein the Ti precursor flow rate is 100 sccm to 5000 sccm. 13. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: exposing a semiconductor substrate to a Ti precursor at a Ti precursor flow rate and forming a thin film of TiN on the semiconductor substrate at one or more periodic vapor deposition cycles of N precursor flow rate to N precursor exposure, wherein the N precursor flow rate exceeds 500 sccm, and wherein the method forms a The TiN thin film of crystalline texture makes the X-ray spectrum of the TiN thin film have the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN The peak height or intensity of the peaks exceeds the ratio of 0.4. 14. As in the method of embodiment 13, the ratio of the flow rate of the N precursor to the flow rate of the Ti precursor (N/Ti flow ratio) is 3-100. 15. The method of embodiment 14, wherein the method makes increasing the N/Ti flow ratio reduce the thickness of the TiN film. 16. The method of embodiment 15, wherein reducing the thickness reduces the resistivity of the TiN thin film. 17. The method of any one of embodiments 15-16, wherein reducing the thickness increases the Young's modulus of the TiN thin film. 18. The method of embodiment 17, wherein increasing the Young's modulus comprises increasing to a value exceeding 150 GPa. 19. The method of any one of embodiments 15 to 18, wherein reducing the thickness increases the hardness of the TiN film. 20. The method of embodiment 19, wherein increasing the hardness comprises increasing to a value exceeding 6 GPa. 21. The method of any one of embodiments 15 to 20, wherein reducing the thickness reduces the chlorine content of the TiN thin film. 22. The method according to any one of embodiments 13 to 21, wherein reducing the deposition pressure increases the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the difference between the (200) crystal orientation corresponding to TiN This ratio of the peak heights or intensities of X-ray diffraction peaks. 23. The method of any one of embodiments 13 to 22, wherein the N precursor flow rate is 500 sccm to 10,000 sccm. 24. The method of any one of embodiments 13 to 23, wherein the Ti precursor flow rate is 100 sccm to 5000 sccm. 25. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: exposing a semiconductor substrate to each comprising a first Ti precursor at a first Ti precursor flow rate body and one or more first periodic vapor deposition cycles of exposure to the first N precursor flow rate to the first N precursor to form a first TiN thin film on the semiconductor substrate, by making the semiconductor Exposing the substrate to one or more second periodic vapor depositions each comprising exposure to the second Ti precursor at a second Ti precursor flow rate and exposure to the second N precursor at a second N precursor flow rate cyclically forming a second TiN film on the first TiN film, wherein the method causes one or both of the first and second TiN films to have a preferential (111) crystalline texture such that the first and second TiN films The X-ray spectrum of one or both of the films has a peak height or intensity of an X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and a peak height or intensity of an X-ray diffraction peak corresponding to the (200) crystal orientation of TiN or The intensity exceeds the ratio of 0.4. 26. The method of embodiment 25, wherein relative to the corresponding exposure to one or both of the first Ti precursor and the first N precursor during the one or more first periodic vapor deposition cycles, Exposure to one or both of the second Ti precursor and the second N precursor during the one or more second periodic vapor deposition cycles is at a higher pressure. 27. The method of embodiment 26, the first ratio of the first N precursor flow rate to the first Ti precursor flow rate (first N/Ti flow ratio) and the second N precursor flow rate to the One or both of the second ratio of the second Ti precursor flow rate (second N/Ti flow ratio) is 3-100. 28. The method of embodiment 27, wherein the method causes increasing one or both of the first N/Ti flow ratio and the second N/Ti flow ratio to decrease one or both of the first and second TiN films The corresponding thickness of the two. 29. The method of embodiment 28, wherein reducing the corresponding thicknesses reduces the corresponding resistivity of one or both of the first and second TiN thin films. 30. The method of embodiment 28 or 29, wherein reducing the corresponding thicknesses increases the corresponding Young's modulus of one or both of the first and second TiN thin films. 31. The method of embodiment 30, wherein increasing the Young's moduli comprises increasing to a value exceeding 150 GPa. 32. The method of any one of embodiments 28 to 31, wherein decreasing the corresponding thicknesses increases the corresponding hardness values of the TiN thin film and the second TiN thin film. 33. The method of embodiment 32, wherein increasing the hardness values comprises increasing to a value exceeding 6 GPa. 34. The method of any one of embodiments 28 to 33, wherein reducing the corresponding thicknesses reduces the corresponding chlorine contents of the first and second TiN thin films. 35. The method according to any one of embodiments 25 to 34, wherein for the TiN thin film, the peak height or the intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN is the same as that corresponding to the TiN The ratio of the peak height or the intensity of the X-ray diffraction peak of (200) crystal orientation is higher relative to the ratio for the second TiN thin film. 36. The method of any one of embodiments 25 to 35, wherein during the one or more first periodic vapor deposition cycles, one or both of the first Ti precursor and the first N precursor The exposures are at a reactor pressure of less than about 5 Torr, and wherein during the one or more second periodic vapor deposition cycles to one or the second Ti precursor and the second N precursor Both such exposures were at reactor pressures greater than about 5 Torr. 37. A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: exposing a semiconductor substrate to each comprising a first Ti precursor at a first Ti precursor flow rate forming a first TiN thin film on the semiconductor substrate at a first pressure by exposure of a precursor and one or more first periodic vapor deposition cycles of exposure to the first N precursor at a first N precursor flow rate, Wherein the first TiN thin film has a crystalline texture, so that the X-ray spectrum of the first TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) crystal orientation corresponding to TiN The ratio of the peak heights or intensities of the X-ray diffraction peaks exceeding 0.4; and by exposing the semiconductor substrate to each comprising exposure to the second Ti precursor at a second Ti precursor flow rate and a second N precursor flow One or more second periodic vapor deposition cycles of exposure to a second N precursor to form a second TiN film on the first TiN film at a second pressure higher than the first pressure. 38. The method of embodiment 37, wherein the second pressure is greater than 5 Torr. 39. The method according to embodiment 37 or 38, wherein the second TiN thin film has a crystalline texture such that the X-ray spectrum of the second TiN thin film has a peak height corresponding to the X-ray diffraction peak of the (111) crystal orientation of TiN or The ratio of the intensity to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN is lower than the corresponding ratio of the first TiN thin film. 40. The method of any one of embodiments 37 to 39, wherein at least a first ratio of the first N precursor flow rate to the first Ti precursor flow rate (first N/Ti flow ratio) is from 3 to 100. 41. The method of embodiment 40, wherein a second ratio of the second N precursor flow rate to the second Ti precursor flow rate (second N/Ti flow ratio) is lower than the first N/Ti flow rate Compare. 42. The method of embodiment 41, wherein the method causes increasing one or both of the first N/Ti flow ratio and the second N/Ti flow ratio to decrease one or both of the first and second TiN films The corresponding thickness of the two. 43. The method of embodiment 42, wherein reducing the corresponding thicknesses reduces the corresponding resistivity of one or both of the first and second TiN thin films. 44. The method of embodiment 42, wherein reducing the corresponding thicknesses increases the corresponding Young's modulus of one or both of the first and second TiN thin films. 45. The method of embodiment 44, wherein increasing the Young's moduli comprises increasing to a value exceeding 150 GPa. 46. The method of embodiment 42, wherein decreasing the corresponding thicknesses increases the corresponding hardness values of one or both of the first and second TiN thin films. 47. The method of embodiment 46, wherein increasing the hardness values comprises increasing to a value exceeding 6 GPa. 48. The method of embodiment 42, wherein reducing the corresponding thicknesses reduces the corresponding chlorine contents of the first and second TiN thin films. 49. The method of embodiment 37, wherein the first pressure is less than 5 Torr.

儘管本文中已參考特定實施例描述本發明,但此等實施例並不用於限制本發明且係出於闡釋性目的而闡述。熟習此項技術者將明白,可在不脫離本發明之精神及範疇之情況下進行修改及改良。While the invention has been described herein with reference to specific embodiments, these embodiments are not intended to limit the invention and are set forth for illustrative purposes. Those skilled in the art will appreciate that modifications and improvements can be made without departing from the spirit and scope of the invention.

本文中所揭示之各項實施例之此等簡單修改及改良係在本發明之範疇內,且此外,本發明之特定範疇將藉由隨附發明申請專利範圍予以定義。Such simple modifications and improvements of the various embodiments disclosed herein are within the scope of the invention, and furthermore, the specific scope of the invention will be defined by the accompanying claims.

在前文中,將瞭解,實施例之任一者之任何特徵可與實施例之任何其他者之任何其他特徵組合或用實施例之任何其他者之任何其他特徵組合置換。In the foregoing, it will be appreciated that any feature of any one of the embodiments may be combined with or replaced by any other combination of features of any other of the embodiments.

除非背景內容另有清楚要求,否者在描述及發明申請專利範圍各處,字詞「包括(comprise/comprising)」、「包含(include/including)」及類似者應解釋為包含意義,與排他性或詳盡性意義相反;即,解釋為「包含但不限於」之意義。如本文中通常所使用,字詞「耦合」係指可直接連接或藉由一或多個中間元件連接之兩個或兩個以上元件。同樣地,如本文中通常所使用,字詞「連接」係指可直接連接或藉由一或多個中間元件連接之兩個或兩個以上元件。此外,字詞「在本文中」、「在上文」、「在下文」及類似含義之字詞在於本申請案中使用時應係指本申請案整體而非指本申請案之任何特定部分。在背景內容允許之情況下,上文[實施方式]中之使用單數或複數之字詞亦可分別包含複數或單數。關於兩個或兩個以上品項之清單之字詞「或」,該字詞涵蓋所有以下字詞解釋:該清單中之品項之任一者、該清單中之所有品項及該清單中之品項之任何組合。Unless the context clearly requires otherwise, throughout the description and claims, the words "comprise/comprising", "include/including" and the like shall be construed as inclusive, and exclusive Or the opposite meaning of exhaustiveness; that is, interpreted as the meaning of "including but not limited to". As generally used herein, the word "coupled" refers to two or more elements that may be connected directly or through one or more intervening elements. Likewise, as generally used herein, the word "connected" refers to two or more elements that may be connected directly or through one or more intervening elements. Additionally, the words "herein," "above," "hereafter," and words of similar import, when used in this application, shall refer to this application as a whole and not to any particular portions of this application. . Where the background content permits, the above [embodiment] words using singular or plural may also include plural or singular respectively. The word "or" in a list of two or more items includes all interpretations of the following words: any of the items in the list, all items in the list, and any combination of items.

此外,除非另有明確陳述或在如所使用之背景內容內以其他方式理解,否則本文中使用之條件語言(尤其諸如「可以(can/could)」、「可能(might)」、「可(may)」、「例如(e.g./for example)」、「諸如」及類似者)一般意欲傳達某些實施例包含而其他實施例不包含特定特徵、元件及/或狀態。因此,此條件語言一般並不意欲暗示一或多項實施例在任何情況下需要特徵、元件及/或狀態,或此等特徵、元件及/或狀態是否包含於任何特定實施例中或在任何特定實施例中執行。Furthermore, unless expressly stated otherwise or otherwise understood within the context as used, conditional language (especially words such as "can/could", "might", "could ( "may", "e.g./for example", "such as" and the like) are generally intended to convey that some embodiments include and other embodiments do not include a particular feature, element, and/or state. Accordingly, this conditional language is generally not intended to imply that one or more embodiments require a feature, element, and/or state in any instance, or whether such feature, element, and/or state is included in any particular embodiment or in any particular implemented in the example.

雖然已描述某些實施例,但此等實施例僅藉由實例呈現,且並不意欲限制本發明之範疇。實際上,本文中所描述之新穎設備、方法及系統可依多種其他形式體現;此外,可在不脫離本發明之精神之情況下在本文中所描述之方法及系統之形式上作出各種省略、置換及改變。例如,雖然以給定配置呈現特徵,但替代實施例可用不同組件及/或感測器形貌執行類似功能性,且可刪除、移動、添加、細分、組合及/或修改一些特徵。此等特徵之各者可依多種不同方式實施。可組合上文所描述之各項實施例之元件及動作之任何合適組合以提供進一步實施例。上文所描述之各種特徵及程序可彼此獨立地實施,或可以各種方式組合。本發明之特徵之所有可能組合及子組合意欲落在本發明之範疇內。While certain embodiments have been described, these embodiments have been presented by way of example only, and are not intended to limit the scope of the inventions. Indeed, the novel devices, methods, and systems described herein may be embodied in many other forms; furthermore, various omissions, forms, and forms of the methods and systems described herein may be made without departing from the spirit of the invention. Substitution and change. For example, although features are presented in a given configuration, alternative embodiments may perform similar functionality with different components and/or sensor topography, and some features may be deleted, moved, added, subdivided, combined, and/or modified. Each of these features can be implemented in a variety of different ways. Any suitable combination of the elements and acts of the various embodiments described above may be combined to provide further embodiments. The various features and procedures described above can be implemented independently of each other, or can be combined in various ways. All possible combinations and subcombinations of features of the invention are intended to fall within the scope of the invention.

100:基板 104:前驅體分子/經吸附分子 108:層 112:層 116:相對平滑二維層/穩定二維層 120:薄膜結構 300:原子層沈積方法/方法 310:步驟 320:步驟 330:步驟 350:半導體結構/半導體薄膜結構 360:基板 370:第一部分 380:第二部分 400A:第一循環/第一原子層沈積(ALD)循環 400B:第二循環/第二原子層沈積(ALD)循環 404:暴露 404A:分壓力上升狀態 404B:主暴露狀態 404C:分壓力下降狀態 404P:總反應腔室壓力/總壓力 408:暴露 408A:分壓力上升狀態 408B:主暴露狀態 408C:分壓力下降狀態 408P:總反應腔室壓力/總壓力 412:暴露 412A:分壓力上升狀態 412B:主暴露狀態 412C:分壓力下降狀態 412P:總反應腔室壓力/總壓力 416:暴露 416A:分壓力上升狀態 416B:主暴露狀態 416C:分壓力下降狀態 416P:總反應腔室壓力/總壓力 500:半導體結構 504:半導體基板/底層半導體 508:介電質層 512:TiN層 512A:薄膜 512B:薄膜 512C:薄膜 516:高縱橫比結構 604:均方根(RMS)表面粗糙度趨勢 608:階梯覆蓋率趨勢 904:經量測階梯覆蓋率 908:經量測階梯覆蓋率 1000:半導體裝置 1004:基板 1008:介電質層 1012:阻障層 1016:接觸插塞 1100:原子層沈積方法/方法 1110:步驟 1120:步驟 1130:步驟 100: Substrate 104: Precursor molecules/adsorbed molecules 108: layers 112: layer 116: Relatively smooth two-dimensional layer / stable two-dimensional layer 120: thin film structure 300: Atomic Layer Deposition Methods/Methods 310: step 320: Step 330: Step 350: Semiconductor Structure/Semiconductor Thin Film Structure 360: Substrate 370: Part One 380: Part Two 400A: First Cycle/First Atomic Layer Deposition (ALD) Cycle 400B: Second Cycle/Second Atomic Layer Deposition (ALD) Cycle 404: exposed 404A: Partial pressure rising state 404B: Main Exposure Status 404C: Partial pressure drop state 404P: total reaction chamber pressure/total pressure 408: exposed 408A: Partial pressure rising state 408B: Main Exposure Status 408C: Partial pressure drop state 408P: total reaction chamber pressure/total pressure 412: exposed 412A: Partial pressure rising state 412B: Main Exposure Status 412C: Partial pressure drop state 412P: total reaction chamber pressure/total pressure 416: exposed 416A: Partial pressure rising state 416B: Main Exposure Status 416C: Partial pressure drop state 416P: total reaction chamber pressure/total pressure 500: Semiconductor Structures 504: Semiconductor substrate / underlying semiconductor 508: dielectric layer 512: TiN layer 512A: Film 512B: Film 512C: Film 516: High aspect ratio structure 604: Root Mean Square (RMS) Surface Roughness Trend 608: Ladder Coverage Trends 904: Measured step coverage 908: Measured step coverage 1000: Semiconductor device 1004: Substrate 1008: dielectric layer 1012: barrier layer 1016: contact plug 1100: Atomic layer deposition methods/methods 1110:step 1120: Step 1130: Step

圖1A至圖1D示意性地繪示在不同生長模式下之薄膜之成核及生長機制。1A to 1D schematically illustrate the nucleation and growth mechanisms of thin films under different growth modes.

圖2係藉由熱原子層沈積生長於經氧化物塗佈之矽基板上之TiN層之橫截面透射電子顯微照片。Figure 2 is a cross-sectional transmission electron micrograph of a TiN layer grown by thermal atomic layer deposition on an oxide-coated silicon substrate.

圖3A係示意性地繪示根據實施例之藉由使基板暴露至具有不同對應前驅體暴露壓力之複數個循環來形成TiN層之原子層沈積方法的流程圖。3A schematically depicts a flowchart of an atomic layer deposition method for forming a TiN layer by exposing a substrate to a plurality of cycles with different corresponding precursor exposure pressures, according to an embodiment.

圖3B示意性地繪示根據實施例之包括藉由其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法形成之TiN層之半導體結構的橫截面視圖。3B schematically depicts a cross-sectional view of a semiconductor structure including a TiN layer formed by an atomic layer deposition method in which a substrate is exposed to a plurality of cycles with different corresponding precursor exposure pressures, according to an embodiment.

圖4示意性地繪示根據實施例之其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法之不同循環的壓力跡線。4 schematically depicts pressure traces for different cycles of an atomic layer deposition method in which a substrate is exposed to a plurality of cycles with different corresponding precursor exposure pressures, according to an embodiment.

圖5示意性地繪示用在通孔之不同部分處具有不同厚度之TiN層加襯裡之該通孔的橫截面視圖。Figure 5 schematically depicts a cross-sectional view of a via lined with a TiN layer having different thicknesses at different parts of the via.

圖6係展示根據實施例之藉由其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法形成之TiN層之依據厚度而變化之實驗量測之表面粗糙度及階梯覆蓋率趨勢的圖表。6 shows experimentally measured surface roughness and steps as a function of thickness for a TiN layer formed by an atomic layer deposition method in which a substrate is exposed to multiple cycles with different corresponding precursor exposure pressures, according to an embodiment. A graph of reach trends.

圖7A係用藉由其中使基板暴露至在相同前驅體暴露壓力下執行之ALD循環之原子層沈積方法形成之TiN層加襯裡之高縱橫比通孔的橫截面透射電子顯微照片。7A is a cross-sectional transmission electron micrograph of a TiN layer lined high aspect ratio via formed by an atomic layer deposition method in which the substrate is exposed to ALD cycles performed at the same precursor exposure pressure.

圖7B係圖7A中所展示之高縱橫比通孔之上區域之橫截面透射電子顯微照片。Figure 7B is a cross-sectional transmission electron micrograph of the region above the high aspect ratio via shown in Figure 7A.

圖7C係圖7A中所展示之高縱橫比通孔之下區域之橫截面透射電子顯微照片。Figure 7C is a cross-sectional transmission electron micrograph of the region under the high aspect ratio via shown in Figure 7A.

圖8A係根據實施例之藉由其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法在類似於圖7A中所展示之高縱橫比通孔之高縱橫比通孔之上區域處形成之TiN層的橫截面透射電子顯微照片。8A is a high aspect ratio via similar to that shown in FIG. 7A by an atomic layer deposition method in which the substrate is exposed to multiple cycles with different corresponding precursor exposure pressures, according to an embodiment. Cross-sectional transmission electron micrograph of the TiN layer formed at the upper region.

圖8B係形成在圖8A中所展示之高縱橫比通孔溝渠之下區域處之TiN層的橫截面透射電子顯微照片。8B is a cross-sectional transmission electron micrograph of a TiN layer formed at the region under the high aspect ratio via trench shown in FIG. 8A.

圖9係展示根據實施例之在單一暴露壓力下藉由原子層沈積形成之TiN層與在複數個暴露壓力下藉由原子層沈積形成之TiN層之間的經量測階梯覆蓋率之統計比較的圖表。9 shows a statistical comparison of measured step coverage between TiN layers formed by ALD at a single exposure pressure and TiN layers formed by ALD at multiple exposure pressures, according to embodiments. chart.

圖10示意性地繪示根據實施例之用藉由其中使基板暴露至具有不同對應前驅體暴露壓力之複數個循環之原子層沈積方法形成之TiN層加襯裡之通孔的橫截面視圖。10 schematically depicts a cross-sectional view of a TiN layer-lined via formed by an atomic layer deposition method in which a substrate is exposed to a plurality of cycles with different corresponding precursor exposure pressures, according to an embodiment.

圖11係示意性地繪示根據實施例之藉由使基板暴露至相對較高N前驅體流動速率而形成具有增加之(111)結晶紋理之TiN層之原子層沈積方法的流程圖。11 schematically depicts a flowchart of an atomic layer deposition method for forming a TiN layer with increased (111) crystalline texture by exposing a substrate to a relatively high N precursor flow rate, according to an embodiment.

圖12A繪示根據實施例之具有不同程度之(111)結晶紋理之TiN薄膜之實驗X射線繞射光譜。FIG. 12A shows experimental X-ray diffraction spectra of TiN thin films with different degrees of (111) crystalline texture according to embodiments.

圖12B係繪示自圖12A之X射線繞射光譜獲得之對應於TiN之(111)晶向之X射線繞射峰之峰值高度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度之實驗比率的圖表。FIG. 12B shows the peak height of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the peak value of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN obtained from the X-ray diffraction spectrum of FIG. 12A Graph of the experimental ratio of height.

圖13係根據實施例之具有增加之(111)結晶紋理之TiN薄膜之實驗厚度及電阻率量測值的圖表。13 is a graph of experimental thickness and resistivity measurements of TiN films with increased (111) crystalline texture, according to an embodiment.

圖14係根據實施例之具有增加之(111)結晶紋理之TiN薄膜之實驗硬度及模量量測值的圖表。14 is a graph of experimental hardness and modulus measurements of TiN thin films with increased (111) crystalline texture, according to embodiments.

圖15係根據實施例之具有增加之(111)結晶紋理之TiN薄膜之實驗硬度量測值的圖表。15 is a graph of experimental hardness measurements of TiN thin films with increased (111) crystalline texture, according to embodiments.

圖16繪示根據實施例之在不同暴露壓力下形成且具有增加之(111)結晶紋理之TiN薄膜之實驗X射線繞射輪廓。16 shows experimental X-ray diffraction profiles of TiN thin films with increased (111) crystalline texture formed under different exposure pressures according to an embodiment.

圖17繪示根據實施例之具有增加之(111)結晶紋理之TiN薄膜之氯濃度深度輪廓。17 shows the chlorine concentration depth profile of a TiN thin film with increased (111) crystalline texture according to an embodiment.

Claims (49)

一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜,該一或多個週期性氣相沈積循環各包括以Ti前驅體流動速率暴露至Ti前驅體及以N前驅體流動速率暴露至N前驅體, 其中該N前驅體流動速率與該Ti前驅體流動速率之比率(N/Ti流量比)超過3,且 其中該方法形成具有結晶紋理之該TiN薄膜,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: forming a TiN thin film on a semiconductor substrate by exposing the semiconductor substrate to one or more periodic vapor deposition cycles each comprising exposure to a Ti precursor at a Ti precursor flow rate body and exposed to N precursor at the N precursor flow rate, wherein the ratio of the N precursor flow rate to the Ti precursor flow rate (N/Ti flow ratio) exceeds 3, and Wherein the method forms the TiN thin film with crystal texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) crystal orientation corresponding to TiN The ratio of the peak height or intensity of the X-ray diffraction peaks exceeds 0.4. 如請求項1之方法,其中該N/Ti流量比係3至100。The method of claim 1, wherein the N/Ti flow ratio is 3-100. 如請求項2之方法,其中該方法係使得增加該N/Ti流量比減小該TiN薄膜之厚度。The method of claim 2, wherein the method is such that increasing the N/Ti flow ratio reduces the thickness of the TiN film. 如請求項3之方法,其中增加該N/Ti流量比降低該TiN薄膜之電阻率。The method of claim 3, wherein increasing the N/Ti flow ratio reduces the resistivity of the TiN thin film. 如請求項3之方法,其中該方法係使得增加該N/Ti流量比增加該TiN薄膜之楊氏模量。The method of claim 3, wherein the method is such that increasing the N/Ti flow ratio increases the Young's modulus of the TiN thin film. 如請求項5之方法,其中增加該楊氏模量包括增加至超過150 GPa之值。The method of claim 5, wherein increasing the Young's modulus comprises increasing to a value exceeding 150 GPa. 如請求項3之方法,其中該方法係使得增加該N/Ti流量比增加該TiN薄膜之硬度。The method of claim 3, wherein the method is such that increasing the N/Ti flow ratio increases the hardness of the TiN film. 如請求項7之方法,其中增加該硬度包括增加至超過6 GPa之值。The method of claim 7, wherein increasing the hardness comprises increasing to a value exceeding 6 GPa. 如請求項3之方法,其中增加該N/Ti流量比降低該TiN薄膜之氯含量。The method of claim 3, wherein increasing the N/Ti flow ratio reduces the chlorine content of the TiN thin film. 如請求項3之方法,其中該方法係使得降低沈積壓力增加對應於TiN之該(111)晶向之該X射線繞射峰之該峰值高度或該強度與對應於TiN之該(200)晶向之該X射線繞射峰之該峰值高度或該強度之該比率。The method of claim 3, wherein the method is to reduce the deposition pressure to increase the peak height or the intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) crystal orientation corresponding to TiN The peak height of the X-ray diffraction peak or the ratio of the intensity. 如請求項3之方法,其中該N前驅體流動速率係500 sccm至10,000 sccm。The method according to claim 3, wherein the flow rate of the N precursor is 500 sccm to 10,000 sccm. 如請求項3之方法,其中該Ti前驅體流動速率係100 sccm至5000 sccm。The method of claim 3, wherein the Ti precursor flow rate is 100 sccm to 5000 sccm. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至一或多個週期性氣相沈積循環而在該半導體基板上形成TiN薄膜,該一或多個週期性氣相沈積循環各包括以Ti前驅體流動速率暴露至Ti前驅體及以N前驅體流動速率暴露至N前驅體, 其中該N前驅體流動速率超過500 sccm,且 其中該方法形成具有結晶紋理之該TiN薄膜,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: forming a TiN thin film on a semiconductor substrate by exposing the semiconductor substrate to one or more periodic vapor deposition cycles each comprising exposure to a Ti precursor at a Ti precursor flow rate body and exposed to N precursor at the N precursor flow rate, wherein the N precursor flow rate exceeds 500 sccm, and Wherein the method forms the TiN thin film with crystal texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) crystal orientation corresponding to TiN The ratio of the peak height or intensity of the X-ray diffraction peaks exceeds 0.4. 如請求項13之方法,該N前驅體流動速率與該Ti前驅體流動速率之比率(N/Ti流量比)係3至100。As in the method of claim 13, the ratio of the flow rate of the N precursor to the flow rate of the Ti precursor (N/Ti flow ratio) is 3 to 100. 如請求項14之方法,其中該方法係使得增加該N/Ti流量比減小該TiN薄膜之厚度。The method according to claim 14, wherein the method is such that increasing the N/Ti flow ratio reduces the thickness of the TiN film. 如請求項15之方法,其中減小該厚度降低該TiN薄膜之電阻率。The method of claim 15, wherein reducing the thickness reduces the resistivity of the TiN thin film. 如請求項15之方法,其中減小該厚度增加該TiN薄膜之楊氏模量。The method of claim 15, wherein reducing the thickness increases the Young's modulus of the TiN thin film. 如請求項17之方法,其中增加該楊氏模量包括增加至超過150 GPa之值。The method of claim 17, wherein increasing the Young's modulus comprises increasing to a value exceeding 150 GPa. 如請求項15之方法,其中減小該厚度增加該TiN薄膜之硬度。The method of claim 15, wherein reducing the thickness increases the hardness of the TiN thin film. 如請求項19之方法,其中增加該硬度包括增加至超過6 GPa之值。The method of claim 19, wherein increasing the hardness comprises increasing to a value exceeding 6 GPa. 如請求項15之方法,其中減小該厚度降低該TiN薄膜之氯含量。The method of claim 15, wherein reducing the thickness reduces the chlorine content of the TiN thin film. 如請求項15之方法,其中該方法係使得降低沈積壓力增加對應於TiN之該(111)晶向之該X射線繞射峰之該峰值高度或該強度與對應於TiN之該(200)晶向之該X射線繞射峰之該峰值高度或該強度之該比率。The method of claim 15, wherein the method is to reduce the deposition pressure to increase the peak height or the intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the (200) crystal orientation corresponding to TiN The peak height of the X-ray diffraction peak or the ratio of the intensity. 如請求項15之方法,其中該N前驅體流動速率係500 sccm至10,000 sccm。The method according to claim 15, wherein the flow rate of the N precursor is 500 sccm to 10,000 sccm. 如請求項15之方法,其中該Ti前驅體流動速率係100 sccm至5000 sccm。The method of claim 15, wherein the Ti precursor flow rate is 100 sccm to 5000 sccm. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至一或多個第一週期性氣相沈積循環而在該半導體基板上形成第一TiN薄膜,該一或多個第一週期性氣相沈積循環各包括以第一Ti前驅體流動速率暴露至第一Ti前驅體及以第一N前驅體流動速率暴露至第一N前驅體;及 藉由使該半導體基板暴露至一或多個第二週期性氣相沈積循環而在該第一TiN薄膜上形成第二TiN薄膜,該一或多個第二週期性氣相沈積循環各包括以第二Ti前驅體流動速率暴露至第二Ti前驅體及以第二N前驅體流動速率暴露至第二N前驅體, 其中該方法係使得該等第一及第二TiN薄膜之一或兩者具有優先(111)結晶紋理,使得該等第一及第二TiN薄膜之該一或兩者之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率。 A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: forming a first TiN thin film on a semiconductor substrate by exposing the semiconductor substrate to one or more first periodic vapor deposition cycles each comprising a first TiN exposing to the first Ti precursor at the precursor flow rate and to the first N precursor at the first N precursor flow rate; and forming a second TiN film on the first TiN film by exposing the semiconductor substrate to one or more second periodic vapor deposition cycles each comprising Exposure to a second Ti precursor at a second Ti precursor flow rate and exposure to a second N precursor at a second N precursor flow rate, Wherein the method is to make one or both of the first and second TiN films have a preferential (111) crystal texture, so that the X-ray spectrum of the one or both of the first and second TiN films has a corresponding The ratio of the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN exceeds 0.4. 如請求項25之方法,其中相對於在該一或多個第一週期性氣相沈積循環期間之對應暴露至該第一Ti前驅體及該第一N前驅體之一或兩者,在該一或多個第二週期性氣相沈積循環期間之暴露至該第二Ti前驅體及該第二N前驅體之一或兩者係在較高壓力下。The method of claim 25, wherein relative to the corresponding exposure to one or both of the first Ti precursor and the first N precursor during the one or more first periodic vapor deposition cycles, during the Exposure to one or both of the second Ti precursor and the second N precursor during one or more second periodic vapor deposition cycles is at a higher pressure. 如請求項26之方法,該第一N前驅體流動速率與該第一Ti前驅體流動速率之第一比率(第一N/Ti流量比)及該第二N前驅體流動速率與該第二Ti前驅體流動速率之第二比率(第二N/Ti流量比)之一或兩者係3至100。As in the method of claim 26, the first ratio of the first N precursor flow rate to the first Ti precursor flow rate (the first N/Ti flow ratio) and the second N precursor flow rate to the second One or both of the second ratio of the Ti precursor flow rate (second N/Ti flow ratio) is from 3 to 100. 如請求項27之方法,其中該方法係使得增加該第一N/Ti流量比及該第二N/Ti流量比之一或兩者減小該等第一及第二TiN薄膜之一或兩者之對應厚度。The method of claim 27, wherein the method is such that increasing one or both of the first N/Ti flow ratio and the second N/Ti flow ratio reduces one or both of the first and second TiN thin films The corresponding thickness. 如請求項28之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之該一或兩者之對應電阻率。The method of claim 28, wherein reducing the corresponding thicknesses reduces the corresponding resistivity of one or both of the first and second TiN thin films. 如請求項28之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應楊氏模量。The method of claim 28, wherein reducing the corresponding thicknesses increases the corresponding Young's modulus of one or both of the first and second TiN thin films. 如請求項30之方法,其中增加該等楊氏模量包括增加至超過150 GPa之值。The method of claim 30, wherein increasing the Young's modulus comprises increasing to a value exceeding 150 GPa. 如請求項28之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應硬度值。The method of claim 28, wherein reducing the corresponding thicknesses increases the corresponding hardness values of one or both of the first and second TiN thin films. 如請求項32之方法,其中增加該等硬度值包括增加至超過6 GPa之值。The method of claim 32, wherein increasing the hardness values comprises increasing to a value in excess of 6 GPa. 如請求項28之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之對應氯含量。The method of claim 28, wherein reducing the corresponding thicknesses reduces the corresponding chlorine contents of the first and second TiN thin films. 如請求項25之方法,其中針對該第一TiN薄膜,對應於TiN之該(111)晶向之該X射線繞射峰之該峰值高度或該強度與對應於TiN之該(200)晶向之該X射線繞射峰之該峰值高度或該強度之該比率相對於針對該第二TiN薄膜之該比率較高。The method of claim 25, wherein for the first TiN thin film, the peak height or the intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN is in relation to the (200) crystal orientation corresponding to TiN The ratio of the peak height or the intensity of the X-ray diffraction peak is higher relative to the ratio for the second TiN thin film. 如請求項25之方法,其中在該一或多個第一週期性氣相沈積循環期間之該等暴露至該第一Ti前驅體及該第一N前驅體之一或兩者係在小於約5托之第一反應器壓力下,且其中在該一或多個第二週期性氣相沈積循環期間之該等暴露至該第二Ti前驅體及該第二N前驅體之一或兩者係在大於約5托之反應器壓力下。The method of claim 25, wherein the exposure to one or both of the first Ti precursor and the first N precursor during the one or more first periodic vapor deposition cycles is less than about At a first reactor pressure of 5 Torr, and wherein the exposures to one or both of the second Ti precursor and the second N precursor during the one or more second periodic vapor deposition cycles This is at a reactor pressure of greater than about 5 Torr. 一種藉由週期性氣相沈積程序形成包括氮化鈦(TiN)之薄膜之方法,該方法包括: 藉由使半導體基板暴露至一或多個第一週期性氣相沈積循環而在第一壓力下在該半導體基板上形成第一TiN薄膜,該一或多個第一週期性氣相沈積循環各包括以第一Ti前驅體流動速率暴露至第一Ti前驅體及以第一N前驅體流動速率暴露至第一N前驅體, 其中該第一TiN薄膜具有結晶紋理,使得該TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度超過0.4的比率;及 藉由使該半導體基板暴露至一或多個第二週期性氣相沈積循環而在高於該第一壓力之第二壓力下在該第一TiN薄膜上形成第二TiN薄膜,該一或多個第二週期性氣相沈積循環各包括以第二Ti前驅體流動速率暴露至第二Ti前驅體及以第二N前驅體流動速率暴露至第二N前驅體。 A method of forming a thin film comprising titanium nitride (TiN) by a periodic vapor deposition process, the method comprising: forming a first TiN thin film on a semiconductor substrate at a first pressure by exposing the semiconductor substrate to one or more first periodic vapor deposition cycles each comprising exposing to a first Ti precursor at a first Ti precursor flow rate and exposing to a first N precursor at a first N precursor flow rate, Wherein the first TiN thin film has a crystalline texture, so that the X-ray spectrum of the TiN thin film has the peak height or intensity of the X-ray diffraction peak corresponding to the (111) crystal orientation of TiN and the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN. The ratio of peak height or intensity of ray diffraction peaks exceeds 0.4; and forming a second TiN film on the first TiN film at a second pressure higher than the first pressure by exposing the semiconductor substrate to one or more second periodic vapor deposition cycles, the one or more Each of the second periodic vapor deposition cycles includes exposure to a second Ti precursor at a second Ti precursor flow rate and exposure to a second N precursor at a second N precursor flow rate. 如請求項37之方法,其中該第二壓力係大於5托。The method of claim 37, wherein the second pressure is greater than 5 Torr. 如請求項37之方法,其中該第二TiN薄膜具有優先(111)結晶紋理,使得該第二TiN薄膜之X射線光譜具有對應於TiN之(111)晶向之X射線繞射峰之峰值高度或強度與對應於TiN之(200)晶向之X射線繞射峰之峰值高度或強度低於該第一TiN薄膜之該對應比率的比率。The method of claim 37, wherein the second TiN thin film has a preferential (111) crystal texture, so that the X-ray spectrum of the second TiN thin film has a peak height of an X-ray diffraction peak corresponding to the (111) crystal orientation of TiN or The ratio of the intensity to the peak height or intensity of the X-ray diffraction peak corresponding to the (200) crystal orientation of TiN is lower than the corresponding ratio of the first TiN thin film. 如請求項37之方法,其中至少該第一N前驅體流動速率與該第一Ti前驅體流動速率之第一比率(第一N/Ti流量比)係3至100。The method of claim 37, wherein at least a first ratio of the first N precursor flow rate to the first Ti precursor flow rate (first N/Ti flow ratio) is 3-100. 如請求項40之方法,其中該第二N前驅體流動速率與該第二Ti前驅體流動速率之第二比率係(第二N/Ti流量比)低於該第一N/Ti流量比。The method of claim 40, wherein a second ratio of the second N precursor flow rate to the second Ti precursor flow rate (second N/Ti flow ratio) is lower than the first N/Ti flow ratio. 如請求項41之方法,其中該方法係使得增加該第一N/Ti流量比及該第二N/Ti流量比之一或兩者減小該等第一及第二TiN薄膜之一或兩者之對應厚度。The method of claim 41, wherein the method is such that increasing one or both of the first N/Ti flow ratio and the second N/Ti flow ratio decreases one or both of the first and second TiN thin films The corresponding thickness. 如請求項42之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之該一或兩者之對應電阻率。The method of claim 42, wherein reducing the corresponding thicknesses reduces the corresponding resistivity of one or both of the first and second TiN thin films. 如請求項42之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應楊氏模量。The method of claim 42, wherein reducing the corresponding thicknesses increases the corresponding Young's modulus of one or both of the first and second TiN thin films. 如請求項44之方法,其中增加該等楊氏模量包括增加至超過150 GPa之值。The method of claim 44, wherein increasing the Young's modulus comprises increasing to a value exceeding 150 GPa. 如請求項42之方法,其中減小該等對應厚度增加該等第一及第二TiN薄膜之該一或兩者之對應硬度值。The method of claim 42, wherein reducing the corresponding thicknesses increases the corresponding hardness values of one or both of the first and second TiN thin films. 如請求項46之方法,其中增加該等硬度值包括增加至超過6 GPa之值。The method of claim 46, wherein increasing the hardness values comprises increasing to a value exceeding 6 GPa. 如請求項42之方法,其中減小該等對應厚度降低該等第一及第二TiN薄膜之對應氯含量。The method of claim 42, wherein reducing the corresponding thicknesses reduces the corresponding chlorine contents of the first and second TiN thin films. 如請求項37之方法,其中該第一壓力係小於5托。The method of claim 37, wherein the first pressure is less than 5 Torr.
TW110146342A 2020-12-10 2021-12-10 Conformal and smooth titanium nitride layers and methods of forming the same TW202240006A (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US202063123733P 2020-12-10 2020-12-10
US63/123,733 2020-12-10

Publications (1)

Publication Number Publication Date
TW202240006A true TW202240006A (en) 2022-10-16

Family

ID=81974835

Family Applications (1)

Application Number Title Priority Date Filing Date
TW110146342A TW202240006A (en) 2020-12-10 2021-12-10 Conformal and smooth titanium nitride layers and methods of forming the same

Country Status (6)

Country Link
EP (1) EP4259845A4 (en)
JP (1) JP2023552983A (en)
KR (1) KR20230125798A (en)
CN (1) CN116745461A (en)
TW (1) TW202240006A (en)
WO (1) WO2022125820A1 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US12272599B2 (en) 2019-10-08 2025-04-08 Eugenus, Inc. Conformal and smooth titanium nitride layers and methods of forming the same
US12283486B2 (en) 2019-10-08 2025-04-22 Eugenus, Inc. Conformal and smooth titanium nitride layers and methods of forming the same
US11482413B2 (en) 2019-10-08 2022-10-25 Eugenus, Inc. Conformal and smooth titanium nitride layers and methods of forming the same

Family Cites Families (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100439028B1 (en) * 2001-12-27 2004-07-03 삼성전자주식회사 Method for Fabricating Semiconductor Device using two step deposition
US20040013803A1 (en) * 2002-07-16 2004-01-22 Applied Materials, Inc. Formation of titanium nitride films using a cyclical deposition process
US6943097B2 (en) * 2003-08-19 2005-09-13 International Business Machines Corporation Atomic layer deposition of metallic contacts, gates and diffusion barriers
US20060128127A1 (en) * 2004-12-13 2006-06-15 Jung-Hun Seo Method of depositing a metal compound layer and apparatus for depositing a metal compound layer
US20080305561A1 (en) * 2007-06-07 2008-12-11 Shrinivas Govindarajan Methods of controlling film deposition using atomic layer deposition
JP5087657B2 (en) * 2009-08-04 2012-12-05 株式会社日立国際電気 Semiconductor device manufacturing method and substrate processing apparatus
US20110256734A1 (en) * 2010-04-15 2011-10-20 Hausmann Dennis M Silicon nitride films and methods
JP2013133521A (en) * 2011-12-27 2013-07-08 Tokyo Electron Ltd Film deposition method
JP6416031B2 (en) * 2015-03-30 2018-10-31 株式会社Kokusai Electric Semiconductor device manufacturing method, substrate processing apparatus, and program
KR102065243B1 (en) * 2017-05-01 2020-01-10 도쿄엘렉트론가부시키가이샤 Film forming method and film forming apparatus
KR102646467B1 (en) * 2018-03-27 2024-03-11 에이에스엠 아이피 홀딩 비.브이. Method of forming an electrode on a substrate and a semiconductor device structure including an electrode

Also Published As

Publication number Publication date
EP4259845A1 (en) 2023-10-18
WO2022125820A1 (en) 2022-06-16
EP4259845A4 (en) 2024-07-24
JP2023552983A (en) 2023-12-20
CN116745461A (en) 2023-09-12
KR20230125798A (en) 2023-08-29

Similar Documents

Publication Publication Date Title
TWI872126B (en) Conformal and smooth titanium nitride layers and methods of forming the same
US12165918B2 (en) Conformal titanium nitride-based thin films and methods of forming same
US12444603B2 (en) Smooth titanium nitride layers and methods of forming the same
US20250279318A1 (en) Conformal and smooth titanium nitride layers and methods of forming the same
TW202240006A (en) Conformal and smooth titanium nitride layers and methods of forming the same
US12444648B2 (en) Conformal titanium silicon nitride-based thin films and methods of forming same
TW202307249A (en) Conformal titanium silicon nitride-based thin films and methods of forming same
US12431388B2 (en) Conformal titanium silicon nitride-based thin films and methods of forming same
US12283486B2 (en) Conformal and smooth titanium nitride layers and methods of forming the same
TW202244303A (en) Conformal and smooth titanium nitride layers and methods of forming the same
CN117355631A (en) Conformal and smooth titanium nitride layer and method of forming same
CN117378032A (en) Conformal titanium nitride silicon-based film and method of forming same